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== Does this event really cause the other event, according to accepted theory? ==


__TOC__
This question is in regards to the text, "the flow following the upper surface contributes strongly to the downward-turning action."


== Lift force: New Theory of Flight ==
To paraphrase, one event - "the flow follows the upper surface" - causes (or more precisely, is a contributing cause of) a second event - "the air turns downward".


The following information to the reader is being removed by Dolphin51
Is this in accordance with accepted science? If not, I think that the text should be reworded to convey what was meant.


1. There is no commonly accepted explanation of the generation of large lift at small drag of a wing as expressed as late as 2020 in Scientific American as “No one knows what keeps planes in the air”.
I think I may understand the important point that the author was trying to convey. I think the author meant to refer to a baseline of 'atmospheric pressure on all subsurfaces'--which applies when there is no flow--and compare that to the conditions of flight, where the deviation from the baseline is greater on the upper surface than on the lower (so the "contribution" relative to the baseline is mostly from the changed conditions on the upper surface, not the lower as intuition would suggest). But that is very different I think than what was said. The fact is that under conditions of lift, the upper flow is following the surface of the wing, more or less, "because of" (if we must allow a causal interpretation) the excess of pressure from the air above over that applied by the wing. And the pressure on the upper surface of the wing under conditions of lift is opposing, not enhancing lift.


2. Any reference to the peer reviewed published work New Theory of Flight, Journal of Mathematical Fluid Mechanics, 2017, by Hoffman and Johnson, which offers a new explanation, is being removed.
] (]) 23:44, 1 December 2014 (UTC)


What is the motivation to hiding 1 and 2 from the public? ] (]) 07:00, 31 July 2021 (UTC)
:At some point in the article's history, the idea expressed by this passage was followed by some discussion of airflow on both sides of the wing and the point made that some explanations only involve air being deflected by the bottom of the wing. (sometimes called "bullet theroy" or "skipping stone theory"). This was accompanied by a graph showing the pressure distribution along the top and bottom of a wing where the pressure difference along the top was substantially larger than along the bottom. At some point this was excised, whether by accident or not.


:1. The Scientific American article titled “No-one can explain why planes stay in the air” is an article that has been seen here before, and has been analysed in some detail. We weren’t much impressed. See ].
:Which is to say that your interpretation of the ''intent'' is correct. I can see where what is actually written may be interpreted differently than what was meant. A suggestion for how to reword would be welcome. I'll take a look at earlier versions and see if we edited something out that shouldn't have been. Personally, I don't read the passage as a statement of ''cause and effect'' but I can see how someone might interpret it that way. ] (]) 00:24, 2 December 2014 (UTC)


::If you want to initiate a discussion about this Scientific American article you are welcome to do so on this Talk page, but you can see how it has been regarded in the past. ] ''(])'' 07:44, 31 July 2021 (UTC)
:: Sorry, I didn't say why I thought the current text suggested a causal relationship, so I will provide some examples that clarify why I inferred one. (I address this point of yours before answering your good request for proposed wording, since if I'm off a bit in my reading then no change is needed.)


:2. I reverted the following text: ''A New Theory of Flight first presented in Computational Turbulent Incompressible Flow as a new explanation of the generation of large lift at small drag of a wing based on computing turbulent solutions of Euler's equations supported by mathematical analysis, has been developed by J. Hoffman, J. Jansson and C. Johnson.'' See my .
The addition of fertilizer to the poor soil common to the region contributes
strongly to the higher corn yields.
(The sentence implies, for me, that "the addition of fertilizer" is a contributing cause of "higher corn yields")


::This text said almost nothing about the new theory of flight, but it gave prominence to the authors. On Misplaced Pages, the authors of cited sources are not identified in the article, but they should be identified in an in-line citation.
Having three unusually strong candidates for the lower house contributed strongly to the party's gains in that election.
(The sentence implies for me that "having three unusually strong candidates for
the lower house" was a contributing cause of "the party's gains in that election."


::If you are one of Hoffman, Jansson or Johnson, or you have a close association with them, there may be a ].
Adding two extra cylinders to the V6 engine contributed strongly to the increased torque
in the new engine. (The sentence implies, in my reading, that "adding two extra
cylinders to the V6 engine" was a contributing cause of "the increased torque in the new engine".


::There may be a case for adding this information to the article but it should be added in accordance with encyclopaedic standards. I recommend you have a look at some or all of the following:
::*]
::*]
::*]
::*]
::*]


:Regards, ] ''(])'' 08:57, 31 July 2021 (UTC)
In these cases, which are I hope analogous to the text under discussion, it seems that the first event ("addition of fertilizer") is implicitly claimed as being a contributing cause of the second ("increased corn yields").


The book Understanding Aerodynamics by Doug McLean gives hard evidence that a common agreement on a scientific explanation of the generation of large lift at small drag of an airplane wing is missing, as just one piece of evidence to this very remarkable fact expressed in the Scientific American article. Why should Misplaced Pages hide this state affairs from the public?
Does my reading of the original text seem reasonable to you?


Why is any reference to the New Theory of Flight, which gives the first full scientific explanation backed by solid math and computation, , removed?
] (]) 23:38, 7 December 2014 (UTC)


Are you open to a section explaining the essence of the New Theory of Flight? Yes I am one of the authors (Johnson). <!-- Template:Unsigned --><span class="autosigned" style="font-size:85%;">—&nbsp;Preceding ] comment added by ] (] • ]) 08:59, 31 July 2021 (UTC)</span>
:I am not sure there is a significant problem here:


:You have written about a "common agreement on a scientific explanation of ... lift ..." You have also referred to "this very remarkable fact". In the past decades we have seen many examples of people who believe there can only be one truly correct explanation of aerodynamic lift. These people seem to think "my explanation is correct so all other attempts at explanation must be incorrect." Similarly, there is no reason to expect that scientists will reach agreement on one truly correct way to explain aerodynamic lift. The majority of Users who work regularly on the topic of lift reject as nonsense these suggestions that there is only one truly correct explanation of lift. We also reject as nonsense the suggestion that scientists should reach agreement on one explanation of lift, or that there is something mysterious or sinister in the fact that different scientists display expertise in different ways to explain lift.
The higher yields from fertilizer are predicated on it being poor soil. (this is specifically mentioned in the
:The reason your edits have been erased has nothing to do with wishing to hide your theory from public view - it has everything to do with the way it is written and presented in the article. To see how a theory should be written and presented, look closely at the various theories already firmly entrenched in the article - see Sections 2, 4 and 6 in the list of Contents. Also look at the 5 guidance articles I linked in my previous edit. Of course we are open to a section covering a new theory of flight - but it needs to be written in a way that is compatible with the encyclopaedic standards applied across Misplaced Pages. I recommend you draft the section and present it on this Talk page, or on your own personal sandbox, and then use the Talk page to invite interested Users to peruse it and make their comments.
example sentence)
:Please remember to sign your Talk page edits with four tildes. ] ''(])'' 13:06, 31 July 2021 (UTC)
::Your latest addition to the article (see the ) looks like an advertisement for a book or a public lecture, rather than a scholarly entry in an encyclopaedia. It contains no in-line citation of the kind required on Misplaced Pages. You have written "The new theory reveals the true physics of generation of large lift ..." The ''true physics'' - wow, that is a bold claim indeed! It is not an appropriate claim to make on an encyclopaedia, especially when you have correctly revealed that you have a potential conflict of interest in all matters of the New Theory of Lift.
::I suggest you look carefully at the existing content of this article and revise your additions so they look consistent with the rest of the content. ] ''(])'' 13:19, 31 July 2021 (UTC)
:::It also only cites one primary source and a self-published source. According to the manual of style's guidance for ]:
::::Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.


:::So, the latest edit fails to meet basic inclusion criteria. ] (]) 23:06, 31 July 2021 (UTC)
The strong election gains are predicated on the election being for the lower house. (this is not exactly
I appreciate that I can have a discussion with Misplaced Pages on the important scientific question about "what keeps planes on the air" citing Scientific American 2020 reporting that "nobody knows". The fact that this question does not have a proper answer more than 100 years after the take off of powered human flight in 1903 is very remarkable, impossible to understand for the general general public, and kept as a secret kept within the scientific community of fluid dynamics hidden from the public. Yet it is true, and the evidence is massive. There is no convincing theory of flight in the standard scientific literature, and this is clearly evidenced by the Misplaced Pages article on Lift presenting lots of material but no theory claimed to be correct, because there is none. If there was a correct theory, known to be correct, then Misplaced Pages would present this theory and all incorrect theories now being presented would serve no role. The New Theory of Flight is a new scientific theory for the generation of lift at small drag of a wing with massive support from computation and mathematical evidence developed by leading academicians and published in leading peer reviewed journals opening a new window in the AIAA HiLift Workshops. Misplaced Pages can here serve an important role to expose this new theory to the scientific community for scrutiny and the general public for information. Can we agree on this mission?] (]) 18:39, 31 July 2021 (UTC)
mentioned in the example, although the description "that election" might suggest it)


Regarding the Scientific American article, it's a pretty clear case of journalistic malpractice. John D. Anderson said "There is no simple one-liner answer to this...” The author misrepresented his statement as "What Anderson said, however, is that there is actually no agreement on what generates the aerodynamic force known as lift." which is a completely different statement.
The increased torque is predicated on the existing cylinder capacities remaining constant. (this is not mentioned
at all in the example sentence)


This was further compounded by the headline writer (often headlines are written by someone other than the author of the article, so I don't know precisely who to blame here) who turned that into the sensationalist click-bait headline "No One Can Explain Why Planes Stay in the Air" It's utter crap. That said, if the author had turned down the hyperbole there's a decent article there.
The contribution of the upper surface flow is predicted on the downward turning of the upper surface itself. (this
is not mentioned in the example sentence)


Regarding Hoffman et. al. to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. As such it's ]. Perhaps that will change, but until it does, their work doesn't belong in the article. Maybe Doug can add some perspective here.
:Whether these assumptions are made explicit in the given sentence is neither here nor there since they are, one way or another, trivially evident from the overall discussion. One might write, "the flow following the downward-turning upper surface contributes strongly to the downward-turning action of the flow," but I personally think that this would be unnecessarily pedantic. There comes a point where the sheer amount of word salad begins to confuse. Whatever the present version says in terms of phrasing, the physical mechanism it is explaining is obvious enough, and at the end of the day that is what language is for. ] 10:54, 8 December 2014 (UTC)


While it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic, from internal combustion engines to cheese making. There's nothing mysterious going on here - there are very well established models of lift that are quite well understood, at least by practicing aerodynamic professionals. What has happened is that for the better part of the 20th century the most common simple explanation turned out to be just plain wrong, and when that was pointed out, people being human held tightly on to it because nobody ever wants to admit that they were wrong. Much debate and argument followed, with disagreement on how best to take a complex subject and explain it simply. That's very different than "nobody knows" or even "there is no agreement on the (mathematical) theory." Were we to propagate the "nobody knows" shibbolleth we'd be remiss in our duties as wikipedia editors. ] (]) 21:46, 31 July 2021 (UTC)
== Why I now find "The Statment" to be problematic ==


Yes, it is a good idea to call in Doug McLean who has written an excellent book on flight theory with an attempt to come up with something better than the standard theories all know to be incorrect. I have written which I ask you to read and answer the questions posed at the end. Will you do that?] (]) 11:00, 1 August 2021 (UTC)
{{quotation|The resulting force upwards is equal to the time rate of change of momentum of the air deflected downwards.|"The Statement"}}


:Yes, I have read your blog as you requested. I deplore the fact that you have named {{ping|Mr swordfish}} in your blog in the way you have done, presumably without their consent or prior knowledge. This is immature behavior that is unlikely to find any support in the scientific community.
Since I don't know quite where to insert this into the wall of text above I'm starting fresh with a new section. I'm also starting more or less from the beginning. Please bear with me, and thanks in advance for your patience.
:At the end of your blog you ask several questions. All your questions are ]. I'm sure you don't know what a rhetorical question is, so I will explain. A rhetorical question is one that is asked without any genuine expectation of an answer; usually because no answer exists or because no answer is wanted. For example, "Why do we have to endure this horrible Covid pandemic?" is a rhetorical question. In a genuine scientific or philosophical dialogue people say what they mean; they don't ask rhetorical questions.
:I am building a picture of User:SecretofFlight as a somewhat immature and petulant person; someone more interested in advertising his theory than promoting the best quality article on Misplaced Pages. Please grow up or I will stop communicating with you. ] ''(])'' 12:51, 1 August 2021 (UTC)


You say regarding Hoffman et. al to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. You are not well informed. The New Theory is now through Jansson an important discussion point at the collecting world leading competence.


You say that while it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic. This is a misconception about what science is. The main objective of science is to give correct explanations of natural phenomena and it is crucial to distinguish correct theory from false theory. The fact that there is no theory of flight accepted as a correct theory is truly remarkable and efforts to cover up this fact is not science and not in the interest of the public. ] (]) 11:20, 1 August 2021 (UTC)
Let's take a look at a simple model, i.e. a plane flying straight and level at a constant speed. In this model, the only things are the plane, the atmosphere, and the ground. After decomposing the total aerodynamic lift into it's components we have four forces on the plane: lift, drag, weight, and thrust. Lift is opposed by weight and thrust is opposed by drag. Since the plane is flying straight and level L+W=0 and D+T=0. With no net force in either the vertical or horizontal direction, there is no acceleration and consequently no momentum change. For the plane, dp/dt = 0.


I did not get any answer on my question posed on my blog so I repeat it here: Why does Misplaced Pages censor any reference to the well documented New Theory of Flight in a Misplaced Pages article on Lift (force), which is only an account of old theories all known to be incorrect?
The ground, of course, is stationary, so for the ground dp/dt is also zero.
I guess the reason is that the Wikipedians exercising the censorship (Dolphin51 and Mr swordfish) do not themselves carry the scientific expertise required to properly evaluate the merits of the New Theory of Flight and so take the simple way out to dismiss it without any scrutiny. But if so, this is not in the interest of the public. If there is a correct theory of flight, it should not be hidden to the people, in particular not to all people relying on safe air transportation. So I add the following question: Which experts are Misplaced Pages relying on, when dismissing/censoring the New Theory of Flight? ] (]) 18:58, 1 August 2021 (UTC)


:The very simple answer as to why the material was removed is that it does not conform to the various wikipedia policies regarding notability, sourcing, and possibly conflict of interest. Dolphin and I have provided links to the help pages that clearly explain the policies and the reasoning behind them. I would suggest you read them, especially ], ], ], and ] I'd also suggest you drop the allegations of censorship - they just make your case look weak.
The only other thing in the model is the air, and if its momentum is not constant we have a violation of conservation of momentum - how can the air experience a change in momentum without anything else experiencing an equal but opposite change in momentum? So the air (ie the atmosphere as a whole) must have constant momentum, that is dp/dt for the atmosphere as a whole is zero. We don't need to compute integrals of momentum flux and take the limit as the boundary goes to infinity to arrive at this, although making those calculations gives the same result.


:I'm sorry that your theory has apparently not attracted the attention you feel it deserves, but wikipedia is not the place to drum up notoriety. In fact it works exactly the opposite way - first the material must become notable, and only then does it warrant inclusion here. In other words, you need to do your PR work elsewhere first; come back when you have the requisite citations. I'll repeat myself, in case you missed it above:
However, there are subsets of the air that experience non-zero dp/dt. And if we take just the right subset, it can be shown that ''for that subset of the atmosphere'' dp/dt = -L. It is reasonable to interpret the lift physically as the result of the momentum change of that subset of the atmosphere. (not everyone agrees with or likes that interpretation, but it is supported by many reliable sources)


:From ]:
There's nothing special about the vertical direction in the argument above. Looking at the horizontal component of momentum change, thrust is equal in magnitude to drag so the net force in the horizontal direction is zero. For the plane, the horizontal component of dp/dt is zero as well. The ground is just as stationary as it was a couple of paragraphs ago, so we can conclude that for the air the horizontal component of dp/dt is zero.
::Misplaced Pages articles should be based on reliable, published <b>secondary sources</b> and, to a lesser extent, on tertiary sources and primary sources. <b>Secondary or tertiary sources are needed to establish the topic's notability</b> and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.


:One very clear problem with your edits is that you haven't established ''notability''. Feel free to come back when you can. ] (]) 21:30, 1 August 2021 (UTC)
This does not contradict the fact that the propeller or jet is pushing a fairly large amount of air backwards. Unlike with lift, there seems to be no controversy over whether air is pushed backwards by the engine. ( NASA has a concise treatment of thrust and momentum change at http://www.grc.nasa.gov/WWW/k-12/airplane/thrsteq.html). The physics in the horizontal and vertical directions is basically the same - if you take a close look at the propeller blades they're just small airfoils generating lift. One can say that the "real" reason the propeller drives the plane forward is the imbalance of pressure between the front and back of the propeller blades, but most folks are satisfied with the 'push air backwards' idea, so much so that for many simple explanations thrust isn't even explained - most people just get it without any explanation. In any case, looking at the ] of the ] article I don't see any long drawn out discussions about how to explain thrust, the article simply says it's a reaction force and this unremarkable statement has collected few remarks on the talk page.

So what does all this have to do with ''the statement''? Well, one point of the exercise is to show in an easy-to-follow manner that when you consider "the air" as the entire atmosphere then the rate of momentum change of "the air" is zero, not -L. So, if a reader gets the idea that "the air" means the whole atmosphere rather than just a subset then including ''the statement'' as previously worded will give the wrong impression and mislead the reader. However, if we provide context then some version of ''the statement'' would be appropriate.

Another point is to show that dp/dt=0 is not inconsistent with some subset of air being accelerated - either downward as occurs with lift or backwards as occurs with thrust. Some subset of the air is accelerated downward with dp/dt = -L; some subset is being accelerated backwards with dp/dt = -T. I don't know how important it is to specify exactly what subset(s) meets this criteria, but I do think it's important to specify that it is a subset and not the entire atmosphere, that is if we are going to include it at all.

Moving forward, I'll try to collect in one place the cites that relate lift to momentum change of air. then we can put on our wikipedia editor hats and evaluate the material provided by the various reliable sources and perhaps craft a subsection that reflects that material. ] (]) 20:08, 8 December 2014 (UTC)

:The analogy with thrust is a good one. Since a propeller is a rotating aerofoil, there's little difference in the physics, except for geometry.

:I can see why someone familiar with Lanchester's "Principle of No Momentum" might initially see The Statement as a claim that the atmosphere ''as a whole'' is given downwards momentum. The trouble with that interpretation is that for it to be true, the atmosphere would have to fall through the ground. That is a nonsensical assumption, which highlights the straw man in the argument that The Statement is false.

:It's true that momentum can only be calculated for a specified portion of air. I think you've expressed the point well, that that subset of air (and the momentum that is communicated<sup>*</sup> to the rest of the air) exists whether the location of that subset it is specified or not.

:I think we've all agreed from the outset that talking about control volumes at this early stage of the article is more likely to confuse the reader than help them understand how the physical principles expressed in Newton's laws contribute to lift.

:I think once some text for the proposed new section is drafted it will be much easier to agree the facts, and decide what changes (if any) should be made to the section on Newton's laws to improve the coherence of the article as a whole.

:<small></small>
:] (]) 10:15, 9 December 2014 (UTC)

::I'd second that gathering and correlating sources is far the best way forward. And do you know, I have clean forgotten what "the statement" said, it was so long ago. Perhaps it is better not to remind ourselves but to just stick with the sources and a clean sheet? &mdash; Cheers, ] (]) 11:06, 9 December 2014 (UTC)

:::"The atmosphere as a whole" isn't the only definition of "the air" for which a reader is likely to mistakenly think The Statement is true. Another potential trap is the idea that The Statement is true for "the local airflow" in the neighborhood of the foil and that it is only when you look farther afield that other effects creep in. This is a misconception that's been expressed by several participants in this discussion and may still be held by some of them.

:::] seems to have a strange definition of a "straw man". It's obvious to him that The Statement is false for the atmosphere as a whole, so the mentioning of that as an example is a "straw man"? The Statement is also false for "the local airflow", which is perhaps not so obvious. So I disagree with the idea that it's not important to discuss the "location" where this "subset" with dp/dt = -L "exists". I think it's important to know that "the local airflow" isn't that location.

:::In terms of basic physics, a propeller is different from a wing in important ways, and the analogy between thrust and lift is a poor one for the following reasons:

::::* Even in a reference frame moving with the airplane, the propeller blades are moving and doing work on the fluid, leaving behind a slipstream with higher total-pressure than in the rest of the field. In even the simplest model of propeller flow, like Rankine's actuator-disc model from 1859, the boundary of the slipstream is a vortex sheet that has no counterpart in the flow around a 2D lifting foil.

::::* A propeller has a substantial effect on the part of the flow that passes through the disc and becomes the slipstream, and relatively little effect on the rest of the flow. Thus the kind of model used by Clancy and by Chris Waltham, in which only a limited part of the stream is assumed to be affected, applies reasonably well to propeller flow. It doesn't apply so well to the flow around a lifting foil.

::::* Cross-stream pressure gradients play only a minor role in propeller flows but play a key role in the momentum balance in airfoil flows. This is to be expected, given that thrust is a streamwise force, and lift is a cross-stream force.

:::So I don't think analyses of thrust are much help in understanding lift.

:::I also second ]'s initiative to gather the sources.

:::That said, I have some reservations about including direct quotes in the article's list of sources. I understand that it makes things easier for the reader in a way. But it also has a downside. It isn't generally practical to provide a long enough quote to avoid the "out-of-context" problem, and the result can be an incomplete and possibly misleading view of what the quote really represents. In a quote of reasonable length you often get only the author's conclusion, not the assumptions he made or the analysis he used to reach that conclusion. I'd propose that instead of a direct quote we should consider paraphrasing the findings, including a brief summary of the assumptions and methods of analysis.

:::Now that we're collecting sources, I propose that we also collect comments by those who take the time to read the sources, e.g. brief summaries of the models and assumptions that were used, and resulting criticisms etc. My preference would be to append comments directly under each source to make things easy to correlate and to facilitate later discussion.

:::] (]) 01:57, 10 December 2014 (UTC)

::::Yes, I know that there is more than one way to misinterpret The Statement in a way which makes it false. What I'm saying is that the language used is not specific enough to imply ''anything whatsoever'' about how to calculate the rate it describes. I still believe the control volume analyses which account partly for momentum and partly for pressure do not answer the question posed by The Statement. I see that you now describe it as "misleading" rather than "false". The former is an opinion to which you are entitled and I thank you for moderating your language.

::::Personally, I have no problem with the suggestion made above to keep quantitative statements out of the Newtonian section and introduce them later if required. I noticed myself that Langeweische doesn't make any quantitative claims.

::::I look forward to seeing your suggestions for the structure and focus of the new section you propose. ] (]) 17:00, 10 December 2014 (UTC)

::::Doug, I think a big reason why you've received so much pushback here on the talk page about your objection to ''the statement'' is due to the lack of direct quotes from the sources you cite. Citations and ] are what makes the entire wikipedia party happen. While I agree that we need to be careful to not take a single sentence or two out of context, we need more than just a work and a page number to back-up contentious claims.

::::Misplaced Pages can be a funny place sometimes; I'm sure you are quite capable of looking at a page of equations and concluding in words that "these equations clearly show that the time integral of ''foo'' is equal to ''bar''". But unless we have a ] that draws the same conclusion putting that statement into the article is ] or interpretation which is prohibited. If you publish the same statement in a book or a paper we can use it, but if you just say so here on the talk page we can't. Like I say, Misplaced Pages can be a funny place, but those are the rules of evidence.

::::So, I'd prefer to see some direct quotes rather than editors' interpretations. Right now, we have an excerpt from your book and the clarifying aside from Waltham about "doing it right" that we can weigh against the imprecise assertions of Smith and the AAPT committee. Another one or two and we're probably there.

::::Sorry you didn't like the thrust analogy - like any analogy it only goes so far, but I think it serves to illustrate that dp/dt = 0 for the atmosphere as a whole is consistent with non-zero mass flow is some subsets of the atmosphere.

::::Finally (for now) I'd prefer that the raw material thread not be interrupted by a lot of back-and-forth exchanges amongst the editors. Once that starts happening the thread will become difficult to follow. Instead, I'd suggest a sub-thread for each source below the initial post. I'll start with an example. ] (]) 20:45, 10 December 2014 (UTC)


'''Two examples that may help clarify the discussion'''


Consider an ] oriented so that the wind is perpendicular to its centerline with its sail trimmed in and the brake engaged. The sail generates lift which is parallel to the centerline of the boat and the lift force (L) is opposed by the friction force of the brake (B). We'll assume in this idealized model that the brake is strong enough to hold the boat motionless. L + B = 0, the total force on the boat is zero and therefore it's acceleration and dp/dt are zero.

In this model the boat can't move, the ice doesn't move, and the only other thing is the air. Since momentum is conserved, dp<sub>boat</sub>/dt + dp<sub>air</sub>/dt = 0 and the net momentum change of the air is zero.

Now, let's release the brake. If we ignore the negligible friction force of the runners (skates), the net force acting on the boat is L. (drag is opposed by the runners that don't move sideways). If F is the total force on the boat we have F = L = ma = dp<sub>boat</sub>/dt .

Again, conservation of momentum says dp<sub>boat</sub>/dt + dp<sub>air</sub>/dt = 0, and in this case dp<sub>air</sub>/dt = -L. So in this special case we can say that the lift is equal to the time rate of change of momentum of the air.

When we had the brake engaged, the situation was very similar to a plane in steady level flight, with the brake playing the role of gravity in opposing the lift force. When we release the brake, the situation is similar to the idealized model of a wing in an infinite atmosphere in the absence of gravity. In this second situation, ''the statement'' is true even when "the air" is the entire atmosphere. But the usual example when explaining lift is steady level un-accelerated flight in a gravitational field, not a plane flying in the absence of gravity or an iceboat accelerating from a stand still.

To be a bit nit-picky, I should add that in the case of the iceboat, dp<sub>air</sub>/dt = -L is only strictly true for a moment - once it begins accelerating the apparent will will move forward and L will not be parallel to the centerline of the boat anymore so L != dp<sub>boat</sub>/dt in general. Further, since it is accelerating our usual frame of reference will no longer be an inertial reference frame. And eventually the boat will reach a steady speed at which point dp<sub>air</sub>/dt = 0. So I don't think an iceboat accelerating from rest is a good example to place in the article.

Hopefully these two examples (a foil constrained to have no acceleration and a foil that is allowed to accelerate with L being the total net force) will cast a bit of light on how momentum is (or is not) transferred to the air. This thought experiment helped clarify things for me anyway. ] (]) 20:52, 15 December 2014 (UTC)
:You have changed the statement from the version originally stated (and which I copied above before archiving). This change makes the phrase "the air" more ambiguous and easier to attribute an unintended meaning. Have I missed something or is this effectively a new discussion about a new problematic statement? &mdash; Cheers, ] (]) 22:01, 15 December 2014 (UTC)

::Apologies. I didn't recall whether the word "downward" appeared in the original, so I went to the talk page archive to find the earliest example. On July 27th, Doug wrote ''The more specific statement "lift is equal to the time rate of change of momentum of the air" is not correct in general. I recommend deleting this sentence.'' leaving out the word "downward". I mistakenly took this to be the definitive version of ''the statement'' but looking back at the actual draft and subsequent versions of ''the statement'' on the Talk page indicates that the word "downward" was in the original. Thank you for restoring it. ] (]) 22:15, 15 December 2014 (UTC)
:::The version I copied also included the word "deflected". This makes a big difference to what one assumes is the air in question. Without it the Statement is ambiguous and requires a suitable preceding remark to give it context. We have lost that context so, if the Statement as now presented is to mean anything at all that can be discussed, it needs that context restoring. &mdash; Cheers, ] (]) 11:23, 16 December 2014 (UTC)

::::Agree that "downward" needs to be part of the statement, otherwise the air deflected in the horizontal direction by the thrust and drag would be included. However, even with "downward" included the statement is still ambiguous. What is meant by "the air"? If it's the entire atmosphere then the statement is false. If parsed narrowly, the statement says that the total momentum change of all the air with a negative vertical deflection is -L and this does not agree with the results of control volume analysis. If "the air" is a carefully defined subset of the atmosphere then the statement is true, but it's not true for arbitrarily chosen subsets and it's not true for most subsets that one would intuitively choose as representative.

::::Until recently, I was mislead by the statement. Only after reading up a bit on control volume analysis did I realize my intuitive ideas were not supported by rigorous quantitative analysis. I think something like the statement can go into the article if we provide sufficient context, but as it stands it's likely to give the reader the wrong idea. ] (]) 16:06, 16 December 2014 (UTC)

:::::Are the sources which convinced you that your ideas were "not supported by rigorous quantitative analysis" listed below? ] (]) 17:02, 16 December 2014 (UTC)

::::::Yes. Zero net momentum change for the atmosphere as a whole is a fairly standard result. Chapter 8.5 of McLain's book lays it out in words fairly clearly. Google books has a generous excerpt at http://books.google.com/books?id=_DJuEgpmdr8C&q=Manifestations+of+Lift+in+the+Atmosphere+at+Large#v=snippet&q=%22Manifestations%20of%20Lift%20in%20the%20Atmosphere%20at%20Large%22&f=false Here are some quotes:

:::::::"...there is no net downward momentum imparted to the atmosphere as a whole and that the lift is reacted by pressure differences on horizontal planes above and below the wing, or on the ground plane, if there is one. We'll also consider how conservation of momentum applies to control volumes that don't encompass the entire atmosphere. ... the lift can show up at the boundaries either as pressure differences on the horizontal surfaces or as fluxes of vertical momentum mainly through the vertical surfaces, or as combinations of the two, depending on the proportions of the control volume."

:::::::"Prandtl and Tietjens (1934) showed how in steady level flight the lift is balanced by an overpressure on the ground under the airplane, so that of course there is no need for net momentum transfer."

::::::I've been trying to find the actual passage in Prandtl that supports this, but I haven't yet. In any case, I thought that "the air" in ''the statement'' meant the entire atmosphere, or some arbitrary box around the airfoil, but the only interpretation of "the air' that makes the statement true is a tall thin subset of the atmosphere - this is not intuitively obvious. ] (]) 21:11, 16 December 2014 (UTC)

::::::::Thank you for clarifying. Yes, the net change of momentum of the whole atmosphere is zero, but momentum is necessarily imparted to air within the atmosphere. See my comments on the AAPT paper below. ] (]) <span style="font-size: smaller;" class="autosigned"> — Preceding ] comment added 10:06, 17 December 2014 (UTC)</span><!--Template:Undated--> <!--Autosigned by SineBot-->

:::::::::Agreed. The net change of momentum of the whole atmosphere is zero. And within the atmosphere there are subsets which experience non-zero momentum change. If one chooses the subset carefully, the rate of momentum change for that subset is equal to -L. But if one chooses a different subset then in general dp/dt != -L. I think the main point of disagreement is over the lack of precision in referring to that particular carefully chosen subset for which dp/dt = -L as simply "the air" or "the air deflected downward". I'm ok with a bit of imprecision in a qualitative introductory section aimed at the lay person as long as it leaves a basically correct impression. Here, I don't think it leaves a basically correct impression. ] (]) 16:50, 17 December 2014 (UTC)

::::::::::It is imprecise to refer to the ''net'' momentum of a body of air without defining the body, but we don't do that. What is imprecise about saying that momentum is imparted to air within the atmosphere at a rate equal to lift? ] (]) 17:48, 17 December 2014 (UTC)


The only reasonable thing to do is to subject New Theory of Flight to scrutiny by some expert such as Doug McLean. My case is strong because I have hard evidence published in leading journals, while the Misplaced Pages article on Lift (force) is very weak as made very clear in the Talk statement above by Doug. The Misplaced Pages article starts out with (see also ):
"There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift".


This is very serious disinformation Mr Swordfish. Very serious. You apparently agree with the statement above by Anderson: "There is actually no agreement on what generates the aerodynamic force known as lift". You thus know very well that there is no scientific explanation of lift agreed to be correct (only incorrect ones agreed to be incorrect), yet you let Misplaced Pages inform the people of the World that there is one, or even better that there are many although most (all?) of them are incorrect. You must understand that this against the most basic of all Misplaced Pages principles your refer to: Misplaced Pages should not mislead the people. Who is telling you to do that? To cover up what is a fact reported by experts in serious media.
:::::For information, the whole of the disputed section containing what I understand to be "The Statement" can be seen . ] (]) 17:24, 16 December 2014 (UTC)


I want to bring this case to highest level at Misplaced Pages. It is very serious and of great concern to the people. How do I proceed?] (]) 06:54, 2 August 2021 (UTC)
:::::@], I think there is some discussion at cross-purposes here. In saying that "downward" should be included in the Statement, are you implying by omission that "deflected" should ''not'' be? That is the word which you removed and which I am more concerned about. To me, the phrase "the air deflected downward" has a very clear meaning which is garbled when any one word is removed. I cannot help but wonder if it is the removal of "deflected" which might have caused the ambiguity which originally confused you. &mdash; Cheers, ] (]) 19:30, 16 December 2014 (UTC)


::'''User:SecretofFlight''': To bring this case to the highest level of knowledge of physics at Misplaced Pages you should take it to the Physics Project team (see ]). You can do this by posting your case at ]. ] ''(])'' 12:31, 2 August 2021 (UTC)
::::::The word "deflected" does not appear in the AAPT version of The Statement or in any other of the sources, as far as I know. Thus adding "deflected" to it is something that has no citable source. And for what it's worth, it's easy to show (though I know of no citable source for this) that adding "deflected" doesn't make The Statement more correct anyway. There is much more negative dp/dt in the region of "the air deflected downward" than just -L. ] (]) 21:15, 16 December 2014 (UTC)
::Another course of action, which will more likely bring it to the attention of the "highest level", is to raise the issue on one of the various noticeboards. There is a process for resolving disputes that cannot be resolved on the talk page, and I think this one qualifies. See https://en.wikipedia.org/Wikipedia:Noticeboards#List_of_Wikipedia's_noticeboards ] (]) 13:47, 2 August 2021 (UTC)


Thanks for this information. I will now prepare material to take the case New Theory of Flight vs Misplaced Pages Lift (force) to the Physics Project Team and also to Noticeboards.] (]) 16:02, 2 August 2021 (UTC)
::::::No, I'm not implying anything by omission. And removing whatever word I did was an error on my part for which I apologize (I think I removed "downward' but it doesn't really matter).
::::::I disagree that "the air deflected downward" has a clear meaning. If you take it literally then the statement is false. ] (]) 21:24, 16 December 2014 (UTC) :Please post a link here when you have filed your case(s). Thanks. ] (]) 19:11, 2 August 2021 (UTC)
::{{ping|SecretofFlight}} When a dispute exists a User will sometimes post their case in two different places on Misplaced Pages. When this is realised one of the posts gets deleted promptly so Misplaced Pages’s effort is not divided into two places, potentially producing an ambiguous outcome. I suggest you post first on the Project Physics Talk page and see what happens. If you don’t see a suitable outcome after, say a week, then take it to a Dispute Resolution site. If you post at the Dispute site first it is highly likely that you will be asked to raise the matter first with the subject specialists at Project Physics so they have the opportunity to contribute their views, and their views will be highly valued by others who are trying to arbitrate on any dispute. ] ''(])'' 22:26, 2 August 2021 (UTC)
:::::::In Clancy's cylinder model (see below) the air which is deflected downwards is described with mathematical precision. If you take "the affected air" to be the air deflected downwards (and what other interpretation is even remotely plausible?) then the Statement is demonstrably true. So I find your assertions to the contrary to be utterly baffling, an absolute failure between us to establish any common use of language. I get the feeling that we agree on the maths but just not on how to describe it. Still, I don't see how we can take this forward between us, so I guess I will have to withdraw from this conversation. &mdash; Cheers, ] (]) 23:00, 16 December 2014 (UTC)
:::Seems to me that {{ping|SecretofFlight}} has larger issues with how wikipedia makes these kinds of editorial decisions than what is within the normal set of issues that ] deals with. I'm not sure which noticeboard is the best venue to adjudicate this dispute, but my sense is that he will receive a more thorough response at the noticeboards than at ]. But I'll leave it up to him to choose the venue. ] (]) 02:14, 3 August 2021 (UTC)
{{ping|Mr. swordfish,Dolphin51}} Before I take the case further I pose the following basic questions connecting to e.g the Scientific American article with headline "No One Can Explain Why Planes Stay in the Air. Do recent explanations solve the mysteries of aerodynamic lift?" (i) Is this a correct description of the state of the science of lift according to Misplaced Pages? If not, what is incorrect? (ii) Is there an accepted scientific theory/explanation of the generation of lift at small drag of an airplane wing? If yes, which is this theory/explanation?
(iii) Mr. Swordfish states above "It is true that there is no simple, correct, and complete theory of lift". Does this mean that there is a non-simple, correct and complete theory, if so which, or no such thing? (iv) The Misplaced Pages article starts out: "There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift". There seems to be a contradiction between (i)+(ii)+(iii) and (iv), that is a contradiction between the statements (a) There is a commonly accepted scientific explanation of lift, and (b) There is no commonly accepted scientific explanation of lift. Which of (a) and (b) is the view of Misplaced Pages? I want a clear answer, not handwaving that (c) they are both correct since there are many theories carrying different elements, some true some false. It is against this background the New Theory of Flight stands out as the first explanation in both mathematical and physical terms of the generation of lift at small drag of a wing with solid documentation in the scientific literature, which you remove from visibility on Misplaced Pages. The matter is serious. The role of Wikepedia is to give correct information to the people, not double messages that there both is and is not a scientific explanation of lift. Ok?] (]) 06:57, 3 August 2021 (UTC)


:My views on this matter, and my answers to your questions, are all evident in the posts I have made to this thread. I suggest you take your case further. I will respond there. ] ''(])'' 12:40, 3 August 2021 (UTC)
::::::::I have not read Clancy, but I have the book on order. Unfortunately, I have to get it via inter-library loan so probably won't see it until after the new year. It may well be true that in his model the integral of all the air experiencing downward deflection is equal to -L. But from what I've seen in the excerpt posted here, his cylindrical model is not as accurate as the potential flow model. In the potential flow model, a subset of the air experiences dp/dt = -L, but if you add up all the air being deflected downward the magnitude of dp/dt is larger than |L|.
:I agree. We've both already responded to most of this upthread. I fail to see the utility in discussing it further here. ] (]) 13:43, 3 August 2021 (UTC)


{{ping|Mr. swordfish,Dolphin51}} No, you have not answered my questions in your posts! To take the case further it is necessary to make the present standpoint of Misplaced Pages clear on the matter of scientific explanation of lift. You say you will respond in the next instance. I ask you to do this right away, so that we will not have to start all over again. You have a responsibility to all the readers of Misplaced Pages and to the scientific community you are representing to answer my questions. What are your answers? ] (]) 13:59, 3 August 2021 (UTC)
::::::::So, perhaps we are just looking at different models? ] (]) 16:27, 17 December 2014 (UTC)


{{ping|Mr. swordfish,Dolphin51}} If you are unable/unwilling to answer the most basic question concerning the article Lift (force) for which you have responsibility, a question of utter scientific importance, then you are not, as I can see, filling the role of a true Wikipedian, which I think will not be appreciated by Misplaced Pages when made clear in the next instance. Do you see my point? You say that answers are to be found in your posts on this thread. Then point me to them! The world expects clear answers. What are your answers?] (]) 14:34, 3 August 2021 (UTC)
:::::::::Yes, I am sure that we are referencing different models. Some models give dp/dt=0, some 0.5L, some L, some >L. Each model is applicable under different assumptions or conditions, i.e. they are modelling different aspects of the problem, and - crucially to this debate - all are well attested in the literature. Taking a result (or assumption) from one of these aspects of the problem and then complaining that it doesn't match the results derived (or assumed) for a different aspect is at best futile. Asserting that it is therefore "wrong" is nonsensical. If the Statement disturbs you, it is because you and it are addressing different aspects of the problem. &mdash; Cheers, ] (]) 17:49, 17 December 2014 (UTC)


{{ping|Mr. swordfish,Dolphin51}} You can choose between two roles as Wikipedians: (i) You can go to history by opening to a much needed scientific discussion on theory of flight with in particular new input from New Theory of Flight, in a situation where there is no commonly accepted correct scientific theory of flight and all current theories basically dating back more than 100 years, are known to both experts and people through popular science press, to be incorrect/incomplete. (ii) You can act as gate keepers with a cover up that for sure there are (many) theories of flight, that science is settled and that New Theory of Flight has no place on Misplaced Pages. Which role do you prefer? For help to come to a decision I invite you to with in particular the videos and . ] (]) 15:26, 3 August 2021 (UTC)
::::::::::I agree. The idea that ''since these analyses give a numerical value for dp/dt, they all answer exactly the same question'' is tempting, but wrong.
Here is state of art of standard fluid mechanics as expressed by Doug McLean in his book Understanding Aerodynamics concerning scientific understanding of lift:


"So in one sense, the physics of lift is perfectly understood: Lift happens because the flow obeys the NS equations with a no-slip condition on solid surfaces. On the other hand, physical explanations of lift, without math, pose a more difficult problem. Practically everyone, the nontechnical person included, has heard at least one nonmathematical explanation of how an airfoil produces lift when air flows past it. Such explanations fall into several general categories, with many variations. Unfortunately, most of them are either incomplete or wrong in one way or another. And some give up at one point or another and resort to math. This situation is a consequence of the general difficulty of explaining things physically in fluid mechanics, a problem we’ve touched on several times in the preceding chapters."
::::::::::* Lanchester §112 asks, in effect, how much momentum is transferred per unit time between the foil and the ground, via the atmosphere.
::::::::::* Prandtl and Tietjens ask how much overpressure is exerted on the ground due to lift.
::::::::::* The control volume analyses of various other shapes ask how lift can be accounted for by a mixture of pressure and momentum.
::::::::::* The Statement is only concerned with momentum.


We read that generation of lift of a wing is a secret deeply hidden in the Navier-Stokes equations with no slip (but uncomputable because of very thin boundary layer), while scientific understanding in physical terms is a difficult problem, apparently unresolved (as expressed in Proposed revision of simplified explanations of lift below).
::::::::::Just to avoid any confusion, I haven't seen any sources saying |dp/dt| > |L|, has ]. ] (]) 10:56, 18 December 2014 (UTC)


The New Theory of Flight reveals the secret of lift hidden in the Euler/Navier-Stokes equations with slip (without boundary layer and thus computable) in a description of slightly viscous incompressible flow around a long wing as potential flow modified by 3d rotational slip separation at the trailing edge into a turbulent wake, with potential flow generating large lift by attaching to the upper surface while gliding with very small friction as expressed by slip combined with 3d rotational slip separation at the trailing edge without the pressure rise of full potential flow destroying lift.
:::::::::::I think ]'s and ]'s line of argument above mischaracterizes the issue.


In short: Standard CFD as Navier-Stokes with no-slip is uncomputable and hides the secret of lift, while Euler/Navier-Stokes with slip is computable and opens to reveal the true secret in a New Theory of Flight in the form of potential flow modified by 3d rotational slip separation. It is as simple as that. Details on ] (]) 07:48, 2 August 2021 (UTC).
:::::::::::What we're discussing here is the question of how much integrated dp/dt is imparted to the flow by a lifting foil, and as part of that question we're concerned with how dp/dt is distributed in the field.


{{ping|SecretofFlight}} {{ping|Mr swordfish}} {{ping|Dolphin51}} I read "The Secret of Flight" paper and found the description to be compelling but somewhat hyperbolic in its claims. Although this material is not yet covered in secondary sources, it is not fringe, and it is recent and I think sufficiently strong to be included here in the article on lift. I've included a short description towards the end of the article, in Three Dimensional Flow, where it seems to fit best. Please consider keeping it, making changes, or delete it if you think this is not a valuable addition to the article, as I believe it is. ] (]) 21:52, 15 August 2021 (UTC)
:::::::::::Both Clancy's cylinder model and the classical uniform-flow-plus-vortex model address these questions. They are not modeling "different aspects of the problem"; they just model the same flow in different ways. Clancy's model for the velocity field is much more crude than the classical model, and Clancy's model ignores the pressure field, while the classical model models it realistically. Clancy's model assumes dp/dt = -L in the near field (within the cylinder), while finding dp/dt = -L in the classical model requires looking much farther afield (the tall sliver control volume). In this regard, the classical model is realistic, and Clancy's model is not. Comparing the realism of different models in this way is not "futile".


:{{ping|Dilaton}} Thanks for your thoughts on this one. I concede that this new theory might be regarded as sound in some quarters, and might one day be widely accepted among mathematicians as a theory of flight. At present I see nothing to suggest that it is sufficiently mature to warrant mention in Misplaced Pages or any other encyclopaedia aimed at a general audience. We have seen two attempts at describing what this new theory of flight looks like, but I am none the wiser. For example, expressions like:
:::::::::::Lanchester's analysis and the other classical analyses don't deal with momentum exclusively, but they do address the question of dp/dt. In that sense they all address the same question, i.e. the value of integrated dp/dt in the flowfield.
:*''3D vortices''. There appears to be nothing on Misplaced Pages to explain 3D vortices so this expression cannot be linked to any existing article to enable the reader to find something about these vortices. (Is this just an alternative to line vortex or vortex filament? Or is it somehow different?)
:* ''potential flow modified by 3D rotational slip separation at the trailing edge into a turbulent wake''. This is inaccessible to a general audience. It looks like something from a PhD thesis. Misplaced Pages is not the place for such a thesis.
:* ''the potential flow generates large lift by attaching to the upper surface while allowing a wing to glide with very small drag from turbulent vortex attachment at the trailing edge.'' Potential flow attached to the upper surface? Surely every application of potential flow around an airfoil since the time of d’Alembert has assumed the flow is attached to the upper surface, and to the lower surface as well? Sentences like this serve more to confuse than to explain.
:If it is to earn a place in this article, it must be described in a way that a general audience might comprehend. Despite your best efforts, your recent addition to the article is unlikely to be comprehended by a specialist audience of fluid-dynamic-literate users, much less by a general audience.
:My view is that your recent addition should be removed. I will wait to see what {{u|Mr swordfish}} and other Users think. ] ''(])'' 07:35, 16 August 2021 (UTC)


::{{ping|Dolphin51}} Thanks for considering an addition. "3D vortices" is an attempt to convey that these are a collection of vortex filaments of unequal alternating vorticity, with ends attached to the trailing edge. It is essentially a more accurate refinement of the Kutta condition, in which the sheet of shear leaving the trailing edge is now understood as a sheet of turbulent vortices. The improvement of understanding comes in now seeing that this is where the majority of the drag originates on an airfoil. Perhaps the paragraph I attempted to add could be improved with this or other language? ] (]) 15:38, 16 August 2021 (UTC)
:::::::::::True, I have not seen any source saying that control volumes exist for which |dp/dt| > |L|, but it's easy to show that it's true. It's original research and can't be used in the article, but I think it's fair to use as a counterargument against other original research arguments on this page. ] (]) 22:36, 19 December 2014 (UTC)


:Misplaced Pages policy is abundantly clear that there must be secondary sources to include material. So far, there has been none for the "new theory of flight" despite a decades long PR campaign that often spills over into Misplaced Pages. The academic article itself has been accessed about 720 times and has garnered a total of 6 citations in the literature. Now, it may be that as Dolphin says it "...might one day be widely accepted among mathematicians as a theory of flight." but for now it's not. I've removed it since it clearly does not meet the standards for reliably sourced material. ] (]) 14:48, 16 August 2021 (UTC)
== sources relating momentum transfer and lift ==


::{{ping|Mr swordfish}} I understand your concern and respect your adherence to secondary sources; however, ] does state that primary sources published in reliable places can be used with care, and I think this published article may thus qualify and be used carefully. Or we can do as you wish and wait for someone else to write about it. I do think that would be a bit of a loss, as the improvement of understanding of drag from attached vortices seems significant. ] (]) 15:38, 16 August 2021 (UTC)
In this section I'm trying to collect source material for a proposed section on momentum transfer and lift. Additions cheerfully accepted, but let's try to keep extensive discussions out of this thread so we can see what raw material we have to work with.
:::{{ping|Dilaton}}While you are correct that primary sources may be used with care, there must be some secondary sources to support notability. At the risk or repeating what I posted upthread, Misplaced Pages policy on ] says:
::::Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. '''Secondary or tertiary sources are needed to establish the topic's notability''' and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.


:::Here, we have a paper that was published five years ago and in response the world has shrugged. Now, perhaps it is truly the major scientific breakthrough that the authors claim it to be. Perhaps even you agree that it is and think that the world needs to be told about it. Fine. Go do that. But do it somewhere else. Come back when there are sufficient secondary sources to support the notion that it merits inclusion here. ] (]) 23:39, 16 August 2021 (UTC)


I have to say that the sheer volume of debate on these talk pages leads me to believe that the Scientific American article was right after all. --] (]) 05:43, 1 September 2021 (UTC)
<hr>
"What supports an airplane aloft? ... Newton has given us the needed principle in his third law: if the air is to produce an upward force on the wing, the wing must produce a downward force on the air. Because under these circumstances air cannot sustain a force, it is deflected, or accelerated, downward.


:The Scientific American article comprises two distinct elements: firstly there is the title “No-one can explain why planes stay in the air.” and secondly there is the body of the article.
Newton's second law gives us the means for quantifying the lift force:
:My impression of the body of the article is that it contains little to support the title. If you believe the body of the article contains some text addressing what the title says, please let us know what you see - please return to this Talk page and quote the wording you are looking at. Many thanks. ] ''(])'' 05:59, 1 September 2021 (UTC)


== Proposed revision of simplified explanations of lift ==
:F<sub>lift</sub> = m∆v/∆t = ∆(mv)/∆t .


There is a proposal for a revised treatment of simplified explanations of lift available at
The lift force is equal to the time rate of change of the momentum of the air."


https://en.wikipedia.org/User:J_Doug_McLean/sandbox
''Bernoulli and Newton in Fluid Mechanics''<br>
Norman F. Smith<br>
The Physics Teacher 10, 451 (1972); doi: 10.1119/1.2352317<br>
http://dx.doi.org/10.1119/1.2352317


I think in general it is very good. I think it could be improved by addressing the following issues:
<hr>
# The current article states "The downward turning of the flow is not produced solely by the lower surface of the airfoil, and the air flow above the airfoil accounts for much of the downward-turning action." This has been removed in the draft. I think it needs to be stated somewhere in the article, otherwise readers may come away with "skipping stone theory"; I'm not seeing a better place than its current location, but I could be persuaded otherwise.
# it doesn't adequately present the streamtube pinching explanation. Probably most of us reading this are already familiar with this "explanation" which can be found in Anderson and Clancy, but the typical reader will probably have no idea what we're talking about. The current article does present it, and I think if we're going to include this material we should explain it more fully than the draft does.
# it asserts : <blockquote>the "streamtube pinching" explanation also starts by arguing that the flow over the upper surface is faster than the flow over the lower surface</blockquote>That's not my understanding of the argument. In the current version of the article (<s>which I believe accurately reflects the reliable sources</s>) the streamtube pinching explanation starts with the fact that theory predicts and experiments confirm that the streamtubes narrow on the top of the wing, and proceeds from there.
# it lumps streamtube pinching into an "incorrect" subheading, but I'm unconvinced that streamtube pinching is actually incorrect. My view, <s>which I think is born out by the reliable sources</s>, is that it is a correct description of the physical phenomena, but with the logical problem that it begs the question of why the streamtubes change size.
# it claims that speed/Bernoulli explanations come in two basic versions, but there is a third: the half-venturi tube "explanation". There are probably others. I think this can be easily written around, assuming we don't want to drag half-venturi into the article, by replacing "These explanations come in two basic versions" with "There are two common versions of this explanation"
# The final subsection "Alternative explanations, misconceptions, and controversies" is reduced to only one explanation, misconception, or controversy after moving previously contained material upwards. It might be appropriate to address half-venturi, skipping stone, "squeeze the soap" and others here. Or just remove this subsection.


There are probably some other minor edits to avoid repetition and improve readability, but I think if the issues above are addressed the revised material will be ready for publication. Thanks for your efforts on this. ] (]) 00:42, 1 August 2021 (UTC)
"Most of the texts present the Bernoulli formula without derivation, but also with very little explanation. When applied to the lift of an airfoil, the explanation and diagrams are almost always wrong. At least for an introductory course, lift on an airfoil should be
explained simply in terms of Newton’s Third Law, with the thrust up being equal to the time rate of change of momentum of the air downwards. See C. Waltham, “Flight without Bernoulli,”
Phys. Teach. 36, 457 (Nov. 1998)."


:Thanks for the feedback. To respond to the issues raised above:


::1. Yes, let's put this back. And let's find a source to cite for it.
''Quibbles, misunderstandings, and egregious mistakes''<br>
AAPT Physics Textbook Review Committee<br>
Citation: The Physics Teacher 37, 297 (1999); doi: 10.1119/1.880292<br>
http://dx.doi.org/10.1119/1.880292


::2-3. I think the whole paragraph taken together describes the arguments correctly, but I see how it can be confusing if you look at the first sentence by itself. I'll try a rewrite. I don't support retaining the current article's opening statement on what experiments and analyses show. It's a true statement, but no reliable source I know of uses it in the context of a streamtube-pinching explanation of lift, and the current article cites no source for it. My objective is still to stick with the classical sources that propose a reason for the pinching, even if we end up pointing out that the reason doesn't make sense.
<hr>


::4. I agree with your comment on "versions". But I still think streamtube pinching belongs under the "incorrect" heading because its two main steps (streamtube pinching causes higher flow speed, and higher flow speed causes lower pressure) run opposite to actual physical cause-and-effect. In addition to not providing a good reason for the pinching, it has the flaw that conservation of mass isn't a satisfying physical reason why the flow would speed up. Really explaining why something speeds up requires identifying the force that makes it accelerate. I'll add the second "flaw".
"Birds and aircraft fly because they are constantly pushing air downwards:


::5. The upper-surface-as-an-obstacle and the upper-surface-as-a-half-Venturi are really the same argument. Your rewording is OK with me.
:::L=dp/dt (3)


::6. I'm going to try removing the "Alternative explanations..." subhead and move the "Controversy regarding Coanda effect" sub-subhead up with the flow-deflection explanation, as that's the explanation to which it relates.
Here L is the lift force and dp/dt is the rate at which downward momentum is imparted to the airflow...


I've implemented these changes in my sandbox. Thank you for the suggestions. ] (]) 17:23, 4 August 2021 (UTC)
If we were to do this more correctly, we would box in the wing with a control volume of infinite vertical thickness. "


: I have gone through the proposed text and I find it excellent, and an improvement over the current state of the article. I have a few minor language/typographic fixes in mind, which I think will be better carried out once the text is integrated in the article. -- ] (]) 07:09, 5 August 2021 (UTC)
:Thanks for your consideration of my suggestions.
::1. I have added a citation for the assertion that the upper surface produces "much" of the lift. I'd like to find a better one, but I think this will do for now.
::2. My working hypothesis is that the vast majority of our readers will not be familiar with the streamtube pinching explanation. It can be found in Anderson's ''Introduction to Flight, Eighth Edition'', but not in earlier editions (or at least I couldn't find it there), in Clancy's ''Aerodynamics'', and in Eastlake's article for The Physics Teacher. I have been unable to find it elsewhere. A year or so ago I was of the opinion that it was sufficiently obscure that it didn't merit attention in the article, but after acquiring Clancy and seeing it there, my opinion has changed. My best guess is that most people who have taken a college level class in aeronautical engineering have seen it, but it remains mostly unknown to the general population.


::Since we can't expect the reader to already be familiar with it, we should provide a more detailed description - the current draft states "When streamtubes become narrower, conservation of mass requires that flow speed must increase." This is certainly true, but a sentence or two along with a picture will help many readers to understant ''why'' narrow streamtubes imply faster flow.
''Flight without Bernoulli''<br>
C. Waltham<br>
Phys. Teach. 36,457 (Nov. 1998).<br>
http://users.df.uba.ar/sgil/physics_paper_doc/papers_phys/fluids/fly_no_bernoulli.pdf


::3. I think you are correct that the current article's treatment is at variance with the sources. Re-reading Anderson, he starts with "obstruction theory" to explain streamtube pinching, not "Starting with the flow pattern observed in both theory and experiments..." so we should present it his way. Eastlake doesn't explicitly explain why the streamtubes change size, but he alludes to the flow passing "the thickest part of the airfoil" and putting your thumb over the end of a hose, so I'll place him in the "obstruction theory" camp. I don't have my copy of Clancy with me and won't for several weeks, so someone else will need to check that reference.
<hr>


::4. The authors of the current section must have been engaging in an act of charity to re-factor the streamtube pinching explanation so that it is not actually incorrect. Seems that we both agree that the current version is not actually incorrect, but it is different than what is to be found in the cited sources. Since the sources present the explanation as a result of obstruction, we should too. And when we do, I think it is appropriate to lump it under the "Incorrect" heading.
"Now let’s move on to conservation of momentum: the force exerted on a fluid equals the time rate of change (derivative with respect to time) of its linear momentum. If you exert a force on something, you change its momentum. If you don’t exert a force on something, its momentum stays unchanged or is conserved. This is Newton’s laws, if you choose to call it that. When an airfoil is producing lift, that force does in fact change the vertical component of the airflow’s linear momentum, and the drag force changes the horizontal component of the airflow’s linear momentum. ...Measuring lift by measuring the increase in downward vertical velocity in the flow coming off the trailing edge of the airfoil is conceptually possible. This downward velocity is definitely there and is known as downwash. I have never heard of anyone actually measuring it with sufficient precision to calculate lift, not because it is physically unsound but because it is not a practical experiment."


::One thing I'd like to see carried over from the current article is


:::Sometimes a geometrical argument is offered to demonstrate why the streamtubes change size: it is asserted that the top "obstructs" or "constricts" the air more than the bottom, hence narrower streamtubes. For conventional wings that are flat on the bottom and curved on top this makes some intuitive sense. But it does not explain how flat plates, symmetric airfoils, sailboat sails, or conventional airfoils flying upside down can generate lift, and attempts to calculate lift based on the amount of constriction do not predict experimental results.
''An Aerodynamicist’s View of Lift, Bernoulli, and Newton''<br>
Charles N. Eastlake <br>
THE PHYSICS TEACHER Vol. 40, March 2002<br>
http://www.df.uba.ar/users/sgil/physics_paper_doc/papers_phys/fluids/Bernoulli_Newton_lift.pdf


::The material expressed in the first sentence has been carried over, but the rest has not. Since the third sentence above is one of the better (best?) arguments why obstruction theory is lacking I think it makes sense to continue to include it.


::5. Seems to have been taken care of. Thanks.
<hr>
"There is a widespread notion that an airplane in steady level flight continuously imparts net downward momentum to the atmosphere. ... Thinking in intuitive physical terms, we might also expect the impulse imposed by the airplane on the air (the product Lt) to produce a net vertical momentum in the atmosphere that grows with time. This expectation is not satisfied by the mathematics, however. ... If we expected to see a net downward momentum equal to Lt, the result comes as a surprise: The value of the integral over the semi-infinite space above the ground is zero, which means that the airplane imparts no net downward momentum to the atmosphere in steady level flight over a ground plane, regardless of height above the ground."


::6. Moving the Coanda material up and removing the depleted section on "Alternative theories" makes logical sense. My issue with this version of the draft is that the article now spends more time discussing what is essentially a semantic issue than it does treating the much more central idea of lift as a consequence of conservation of momentum. Moving the Coanda material down in the article would be an acceptable solution, but I'm not sure where to move it. Like the streamtube pinching explanation, I think the "Coanda controversy" is limited to folks who have done some formal study or aerodynamics and not widespread in the general population, so perhaps we don't really need to address it. Or perhaps find a more concise way to present it.


::Thanks for considering my suggestions. I think we're making real progress here. ] (]) 14:28, 5 August 2021 (UTC)
''Understanding aerodynamics arguing from the real physics '' sec 8.5<br>
McLean, Doug<br>
Chichester, West Sussex, U.K. : Wiley, 2013.<br>
http://mirlyn.lib.umich.edu/Record/012482734


:::@Mr Swordfish: If at 3. you are alluding to the citation of Clancy p.76 “This lift force ... ... downward momentum of the air” I can confirm that this is an accurate quotation from Section 5.15 ''Lift and Downwash'' (which is on p.76 in my copy.) ] ''(])'' 00:19, 6 August 2021 (UTC)
<hr>
::::@Dolphin: My recollection is that Clancy presents the streamtube pinching explanation, but I don't recall whether he starts with "obstruction theory" or proceeds from some other premise (e.g. the "theory & experiment" approach the article uses). We don't cite Clancy in this subsection, so you'll have to look beyond our citations. If you have your copy handy, I'd appreciate if you could take a look at Clancy's approach and report back. Thanks. ] (]) 18:18, 6 August 2021 (UTC)
On basic control-volume analysis of the rate of change of momentum in a moving fluid:


:::::@Mr Swordfish: I have had a quick look through Clancy. He explains lift using the Circulation Theory and the Kutta-Joukowsky theorem. The book appears to contain no linking of lift on an airfoil and stream tube pinching. There are several diagrams that show streamlines of varying spacing around a circular cylinder with circulation, and around an airfoil-shaped cylinder with different amounts of circulation. In the explanatory text adjacent to the diagram of the circular cylinder with circulation Clancy draws attention to the varying spacing of streamlines and links this to pressure variation using Bernoulli (Section 4.5 ''Circular Cylinder with Circulation'' on p.38) In the text adjacent to diagrams of airfoils Clancy makes no attempt to draw attention to streamline spacing and its implication for pressure.
''The Dynamics and Thermodynamics of Compressible Fluid Flow'' Section 1.5<br>
:::::In para 4.5(b) Clancy writes “The effect of the circulation is generally to increase the speed over the upper surface of the cylinder and to reduce the speed over the lower surface. This effect is shown by the spacing of the streamlines in Fig 4.4”
Shapiro, A. H. 1953. <br>
:::::In para 4.5(c) he writes “From Bernoulli’s Theorem, therefore, it follows that the pressure is generally reduced on the upper surface and increased on the lower surface. As a result, there is a net force vertically upwards. This is lift.” ] ''(])'' 13:49, 7 August 2021 (UTC)
New York: The Ronald Press Company.
::::::I stand corrected about streamtube pinching appearing as an explanation of lift in Clancy. I'm now back to wondering if presenting this explanation here is giving it ]. ] (]) 14:17, 7 August 2021 (UTC)
I've been re-reading the Help article on ], first in the context of the streamtube pinching "explanation", but then in the context of the apparent controversy over the Scientific American article that claims "nobody understands lift". The article on weight states


::Neutrality requires that mainspace articles and pages fairly represent all significant viewpoints that have been published by reliable sources, in proportion to the prominence of each viewpoint in the published, reliable sources. Giving due weight and avoiding giving undue weight means articles should not give minority views or aspects as much of or as detailed a description as more widely held views or widely supported aspects.
McLean: "This analysis shows that for a steady flow the integrated time rate of change of momentum of fluid parcels passing through the interior of a control volume is equal to the integrated (net) flux of momentum through the boundary. This is a basic ingredient in the other analyses cited below."


The current version of the article states succinctly "...there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift." The proposed revision does an about face and states "...neither approach, by itself, is a completely satisfactory explanation." (And then there's the SA article, which I'm going to ignore as ].)


Both of these are valid opinions that are supported by reliable sources. I tend to agree with the latter as my own opinion, but when I put on my editing hat I find it problematical to clearly come down on one side or the other. If we're going to present this controversy, we're supposed to present both sides and "teach the controversy". That said, I don't want to waste our readers' time by rehashing the great Bernoulli v Newton debate that raged back in the late nineties. My preferred solution is to sidestep the issue and avoid sweeping statement about whether both are right, or neither is right, (or whether nobody really knows). The proposed revision clearly explains each approach and its limitations or shortcomings. I think the readers can draw their own conclusions without us having to make sweeping statements like the above examples.
<hr>
For the atmosphere as a whole, including a ground plane:


I'll copy the present proposal over to my sandbox and make the proposed changes there so we retain an easy to access "clean" copy of Doug's proposal.
''Applied Hydro- and Aeromechanics''<br>
Prandtl, L., and O. G. Tietjens. 1934. . New York: Dover Publications. Derivation in connection with figure 150.


Regarding the streamtube pinching, or "obstruction theory", I'm in agreement that it's essentially the same argument as the "half venturi tube" approach, which seems to be more prevalent in the sources so we should give more prominence to it. I'll take a whack at that, along with an attempt to provide a more concise treatment of the Coanda material. ] (]) 13:44, 10 August 2021 (UTC)
McLean: I don't have a copy at hand, so I can't provide a quote, but this is the classic analysis showing that the pressure pattern on the ground constitutes a downward force on the ground, and thus an upward force on the atmosphere, equal to L. The net force on the atmosphere due to the lift, (i.e. the vector sum of the forces exerted by the wing and the ground) is therefore zero, so that the integrated rate of change of vertical momentum for the atmosphere as a whole must be zero.


:My view is that there are multiple explanations of lift, each derived from one or more of the various conservation laws and other laws of physics that are applicable to a solid object immersed in the flow of a fluid. We make use of multiple explanations of lift to serve the needs of the multiple audiences that have an interest in the subject. Even within one audience there are multiple purposes and objectives that cannot be satisfied by just one explanation. For example:
The Prandtl and Tietjens analysis is for the 3D case. It is easy to show that the same overall conclusion applies in 2D. A citable source for the 2D analysis probably exists, but I don't know of one offhand.
:*An explanation of lift that can be presented to 19-year olds will be unsuitable for 13-year olds. An explanation that is both satisfying and satisfactory for student pilots will be unsuitable for students of physics and engineering.
:*An explanation that helps explain lift in 2-dimensional flow will not be satisfactory if the objective is to help explain lift-induced drag.


:I support the sentiment in the present article: “Either can be used to explain lift.” I don’t support the sentiment that "...neither approach, by itself, is a completely satisfactory explanation." It will be unhelpful, unnecessary and unsound to apologise for certain explanations of lift, or to suggest that no satisfactory explanation exists, or that no-one knows what it is. Misplaced Pages is able to demonstrate its maturity and soundness by not engaging in a search for a "completely satisfactory explanation". Nor should Misplaced Pages support a notion that every incomplete explanation must be incorrect.
<hr>
For a circular region centered on the airfoil:


:When we search for the most appropriate explanation of lift for our purposes we are engaging in applied science or applied math or engineering but we aren’t engaging in pure or fundamental science. Bernoulli’s principle and Newton’s laws of motion have universal application and so qualify as fundamental science, but an explanation of lift on an airfoil is simply one of many examples of Bernoulli and Newton in action. There will never be a Committee of eminent scientists whose task is to determine by arbitration the one true explanation of lift.
''Aerodynamic Theory, vol. 1.'' Sections B. V. 6 and B. V. 7.<br>
Durand, W. F., ed. 1932. <br>
New York: Dover Publications.


:When we talk about the explanation of lift based on Bernoulli’s principle, it would really be more accurate to say we are using lift as an example of Bernoulli’s principle in action. Similarly, when we talk about the explanation of lift based on Newton’s laws, it would really be more accurate to say we are using lift as an example of Newton’s laws in action. The pure science is always more fundamental than the application of that science to one of a multitude of everyday observations.
McLean: This is a control-volume analysis of the flow around a 2D lifting body of arbitrary cross-section in an infinite atmosphere, using a circle of large radius as the outer boundary of the volume. It shows that in the far field the flow is independent of the details of the body, and that significant contributions to the pressure and the momentum fluxes at the outer boundary come only from the combination of the uniform flow and the bound vortex. It arrives at a derivation of the Kutta-Joukowski theorem in equation 7.3. Equation 5.6 shows that the flux of vertical momentum across the outer boundary, and thus the time rate of change of vertical momentum in the air in the interior, is equal to only half the lift. Equation 6.6 shows that the integrated vertical pressure force on the outer boundary is upward and equal to half the lift. The net force on the air due to the lift is therefore downward and equal to half the lift, and Newton's second law is satisfied. It is explicitly stated that this result holds regardless of how large the radius of the circle is made.


Reference added by ] (]) 21:08, 16 December 2014 (UTC): :I look forward to seeing your latest proposal on your sandbox. ] ''(])'' 12:10, 11 August 2021 (UTC)
::Dolphin, Agree that different audiences require different explanations, and it is appropriate for us to present several, starting with the easier to understand and proceeding to the more rigorous. I think we need to be careful about using words like "satisfying" and "satisfactory" because they beg the question of "satisfying to whom?" My hunch is that most people are completely satisfied to know nothing about this topic. Those who bother to read the article may come away satisfied after a section or two, or they may read further until they are "satisfied".
::Moving on....


::The opinion “Either can be used to explain lift.” is just that - an ''opinion''. So is the opinion "...neither approach, by itself, is a completely satisfactory explanation." If we're going to include either one, we need to present the other, present both as opinion, and provide some context for how widespread each is in the reliable sources. I'd rather not do that, especially early on in the article. Perhaps a later section on the "Bernoulli v Newton Controversy" would be in order, or perhaps a separate article instead. My preference is to just sidestep it as a distraction and present the various approaches, starting from simple and moving to the complex, with some context to address whatever shortcomings or limitations each approach has. And let the material speak for itself without making unnecessary sweeping generalizations.
An Introduction to Fluid Dynamics
::To that end, I don't think we need the first section "Understanding lift as a physical phenomenon". The article starts with qualitative physical explanations without math and proceeds to the various mathematical models. That is apparent from the table of contents, so I don't think we need to state it explicitly; readers will get it if they bother to read that far. I'm going to remove it from my draft. Comments appreciated.
Batchelor, G. K. 1967
::My view is that no version is 100% complete nor is any version 100% correct. When we do physics, we make abstract models, and in order to make the models tractable we make some simplifying assumptions along the way so the model doesn't exactly describe the actual physical phenomena. That doesn't mean that the models are bad, just that they are always limited, and when criticized for that variance the criticism is often warranted. For instance, 2D potential flow doesn't predict stall, drag, or downwash. But it does a surprisingly good job at predicting lift without making the math impossible. IOW, it's a good but limited model.
Cambridge University Press


::Which is to say that ''every'' explanation is incomplete to some degree. So, I'm not sure it's "fair" to label the explanation based on flow deflection and Newton's laws that way in the title. I do think it's fair to state that it's incomplete in the body, so I'm removing it from the title but leaving it in the body.
Applying the momentum theorem to incompressible inviscid flow around a 2D body of arbitrary cross-section (a general "cylinder") with circulation, and using a control volume bounded by a circle of large radius, Batchelor finds on p. 407:


::Regarding "Bernoulli-based" explanations, the two we discuss in that section are clearly incorrect. Correct explanations involving Bernoulli (or more properly, explanations that are based on models that have some predictive power) always include many other physical principles to the extent that it's a misnomer to call them "Bernoulli-based". To put a finer point on it, they always include conservation of momentum at some level. Bernoulli's principle is just one piece of the puzzle.
"It follows from the calculation of the integral that the side-force exerted by the cylinder appears in the fluid far from the body half as a momentum flux and half in the form of a pressure distribution."
::That said, I think a serious shortcoming of this draft as it stands is that readers may come away with the notion that Bernoulli's principle is somehow wrong, or that it is always incorrect to use it when explaining lift. I think we need so say something along the lines of "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." But I'm not sure where to put it or how best to phrase. Suggestions appreciated. ] (]) 18:32, 14 August 2021 (UTC)


:::UPDATE: I've added "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." to the draft. ] (]) 18:49, 14 August 2021 (UTC)
<hr>
I've not gotten much feedback on the draft in my sandbox. I'm not sure if that's because other editors don't like it, or because they think it's fine as is. Assuming the latter, I'll give it a couple of days and if no objections I'll deploy the material in my sandbox. ] (]) 22:02, 19 August 2021 (UTC)
For rectangular control volumes:
:I will be happy to give some feedback in the next day or two. ] ''(])'' 22:42, 19 August 2021 (UTC)
::Thanks. It's more important that we get it right than that we do it fast. But I want to keep the process moving. ] (]) 01:41, 20 August 2021 (UTC)
:::It looks good to me and I don’t see much to comment on. I have provided my feedback at ]. ] ''(])'' 13:31, 20 August 2021 (UTC)


I think the proposed new section "Understanding lift as a physical phenomenon" is important. It clarifies the status of the qualitative explanations relative to the rigorous scientific understanding embodied in the mathematical theories. In so doing, it says a lot more than what a reader could infer from the TOC or what he would be likely to realize even after reading the entire article. I think it makes what follows much easier to understand.
"For a large rectangular control surface, part of the lift is
attributable to pressure and part to momentum,
depending on the aspect ratio of the surface. For a
square control surface the contributions on the surface
due to momentum and pressure are equal; for a tall, long
vertical surface the contributions are mainly
momentum, while for a streamwise long, flat,
horizontal surface the lift is primarily due to pressure.
This illustrates that it doesn't make much sense to
attribute the lift on an airfoil to either pressure or
momentum effect, unless one takes a control surface on
the actual airfoil surface, when the lift is indisputably
due only to pressure!"


I think we should keep the "Obstruction..." explanation. Anderson is a very prominent author, and this book is a prominent source.


I've put up a new candidate in my sandbox. It avoids the "satisfactory" wording and removes the value judgements from the headings. It also incorporates Swordfish's shortened version of the Coanda section and his separate subheads for "Equal transit time" and "Obstruction...". I added another subhead to separate out the issues common to both explanations that had been swallowed into the "Obstruction..." subsection. I also incorporated his wording on Bernoulli not being incorrect as a principle, with the added qualification that Bernoulli is applicable outside the boundary layer. Comments?
''The facts of lift.'' Section titled "Lift in thin slices: the two dimensional case".<br>
] (]) 19:21, 21 August 2021 (UTC)
Lissaman, P. B. S. 1996. <br>
AIAA 1996-161. <br>
http://arc.aiaa.org/doi/pdf/10.2514/6.1996-161


:I've copied Doug's latest draft over to my sandbox for the purposes of comparison. The diff is here: https://en.wikipedia.org/search/?title=User%3AMr_swordfish%2Fsandbox&type=revision&diff=1040264566&oldid=1039805588 I'll have more to say in a day or so. ] (]) 17:29, 23 August 2021 (UTC)
<hr>
Comments on the latest drafts (24 Aug 2021):
For a tall column of air:


'''o''' The first thing I noticed when looking at the diff was that the latest version from Doug is some 10,000 characters shorter. This is mostly refs that didn't make it over. I don't think it will be controversial to restore the refs, although some may be ripe for pruning. I'll restore all of them in my next draft, and if any are deemed to be unnecessary we can remove them on a case-by-case basis.
"When a loaded aerofoil is dynamically supported by a fluid, we know that its weight is eventually sustained by the surface of the earth, and that the transmission of the stress is effected by the communication of momentum from part to part, and is thereby distributed over a considerable area as a region of increased pressure"


'''o''' Regarding the first section ], it reads to me as an opinion rather than a simple statement of fact. The current version of the article also includes the opinion that "Either can be used to explain lift." I prefer the simple factual statement in my previous draft, which I think adequately foreshadows the qualitative vs mathematical dichotomy to come.
Fig. 62 illustrates the forces on a narrow column of air where W is the weight of the foil acting downwards and the pressure at the base of the column is w. "Consequently the downward momentum imparted per second to the fluid leaving the prism ''plus'' the upward momentum received per second from that entering must be equal to W – w."


:There are several ways to explain how an airfoil generates lift. Some are more complicated or more mathematically rigorous than others; some have been shown to be incorrect. Most simplified explanations follow one of two basic approaches, based either on Newton's laws of motion or on Bernoulli's principle.
"When the height at which the aerofoil is sustained is great in comparison with its own dimensions, the area over which the weight is distributed on the earth's surface is obviously also great, and the quantity w becomes negligible. Under ordinary conditions this would usually be the case, so that the weight may be regarded as in no part statically supported."
'''o''' I looked into other wikipedia articles that link directly to sub-headings, and only found one that would be affected by the current drafts. I added an anchor tag to that section. We should make sure that it makes it into the final version.


'''o''' Agree to keeping the obstruction/constriction/streamtube-pinching explanation. While it's not nearly as widespread as the ETT fallacy, it seems to be common enough for us to reference it here (although I'd be open to an argument that it's not if anyone wants to make it). I think it's worth expending a single sentence on NASA's "Venturi tube" version of it since NASA's site may be the most widely read version.
''Aerodynamics''. §112 – Aerodynamic support<br>
Lanchester F.W. (1907)<br>
Archibald Constable & Co. Ltd.<br>
https://archive.org/stream/aerodynamicscons00lanc#page/146/mode/2up<br>


'''o''' I don't think labeling the incorrect explanation as "incorrect" is a value judgement. Seems to be simply a statement of fact, so I'd advocate restoring that in the titles.
<hr>


'''o''' I like the additional subhead to address issues common to both - I wanted to do that myself, but couldn't come up with a good title.
"The downwash also varies in the streamwise direction. It reaches its ultimate value little more than a chord length behind the trailing edge; and its mean value at the wing itself can be shown to be one half of this ultimate value." (Page 75)


'''o''' I'm unconvinced that it's necessary to state that "Bernoulli's principle is applicable to the flow outside the boundary layer." at this point in the article. I think simply stating "Bernoulli's principle can be used correctly as part of a more complicated explanation of lift." is sufficient for the intended audience for this portion of the article. If we're going to address when Bernoull's principle applies and when it doesn't, that should wait until later in the article.
...


'''o''' Regarding "This explanation is correct as far as it goes but is incomplete. " I've come to agree with Dolphin's ] that "as far as it goes" is a colloquial idiomatic expression, that while common in the US may not be understood the way it's meant to by someone unfamiliar with the expression. If we were writing this for a US audience I'd advocate to keep it, but since we're writing for the broader English-speaking world I think the phrase should be excised.
;5.15 Lift and downwash
We have two candidates for the material at this point:
"The lift produced by a wing is imparted to it through the variations in pressure over its surface. This lift force has its reaction in the downward momentum which is imparted to the air as it flows over the wing. Thus the lift of the wing is equal to the rate of transport of downward momentum of the air.
:This explanation is correct but it is incomplete. It doesn't explain how the airfoil can impart downward turning to a much deeper swath of the flow than it actually touches. Furthermore, it doesn't mention that the lift force is exerted by pressure differences, and doesn't explain how those pressure differences are sustained.


and
"This downward momentum is measured in terms of the induced downwash described above." (Page 76)


:Flow deflection combined with Newton’s laws is a helpful way to explain some aspects of lift. It leaves some questions unanswered; it doesn't explain how the airfoil imparts downward turning to the flow, and it doesn't mention that the lift force is exerted by pressure differences. It doesn't explain how those pressure differences are sustained.
...
I prefer the concise "correct but incomplete" phrasing, but could be persuaded otherwise.


I'll merge the the latest draft from Doug with mine, incorporating the ideas above. Comments as always welcome. ] (]) 16:32, 24 August 2021 (UTC)
"Consider, then, this cylinder of air, as illustrated in Fig. 5.21. The area of cross-section of the cylinder of affected air is 1/4 ''πb''<sup>2</sup>. The rate of mass flow of affected air past the wing is therefore 1/4 ''πρVb''<sup>2</sup>. The rate of transport of downward momentum is therefore 1/4 ''πρVb''<sup>2</sup>''w'', and this must equal the lift, ''L''." (Page 76)


==Oversimplification==
...
The current version of that section still refers to Bernoulli's Principle as "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." This sounds great, but it isnt correct, as it is a (fairly significant) oversimplification of his work. In the context of aviation and aerodynamic lift, it is only accurate along a streamline where no heat is being transferred between the wing and the air. Does the cited work include this gross oversimplification? As importantly, does the gross oversimplification make the concept clearer to the reader? ] (]) 08:26, 23 August 2021 (UTC)


:{{ping|PrimalBlueWolf}} Where you have written “but it isn’t correct ...” do you mean Bernoulli’s principle doesn’t correctly represent the reality; or our article doesn’t correctly reflect the principle described by Bernoulli?
"If we consider unit span of an infinite wing, however, the air above this unit span forms part of a cylinder of infinite radius, and its mass is therefore infinite. Since the downward momentum imparted to the air in unit time is finite, and since the mass of the air is infinite the induced downwash velocity must be zero." (page 77)
:It is well known, and always acknowledged in reliable published sources, that Bernoulli’s principle doesn’t take account of viscous forces within the fluid, nor does it apply to a flow field in which heat is being transferred. Despite these assumptions Bernoulli’s principle is a very powerful tool in analysing the subsonic flows around streamlined bodies. I don’t agree with your characterisation that the Misplaced Pages article represents a “gross oversimplification.” Please explain further. ] ''(])'' 13:57, 23 August 2021 (UTC)


That it doesn't correctly represent the principle as represented in Hydrodynamica. The current version of the article alleges that you can determine velocity and pressure of any other point using Bernoulli's Principle knowing only the velocity and pressure of one point, and the velocity of one other point. That is only valid along a streamline, but the article doesn't acknowledge that. ] (]) 21:25, 23 August 2021 (UTC)
''Aerodynamics'',<br>
Clancy, L.J.<br>
Pitman Publishing (1973)<br>


:It is often stated that "Bernoulli's principle is only valid along a streamline" but this is a misconception. Within a flow field that exhibits uniform flow as the initial condition, BP applies throughout the flow field. This assumes that the energy is constant, i.e. it assumes no heat loss (as one would find in the example of an airplane wing) or no net work done (as one would find in the example of a sailboat). If one is going to pick nits, BP is not applicable to any real world airfoil due to these energy considerations, however it is commonly used as a ''approximation'' or ''simplification'' to make mathematical models tractable. Physics is full of these approximations, e.g. assuming sin(x)=x for sufficiently small x. And if we're not going to assume constant energy, BP doesn't apply along a streamline either.
<hr>


:The statement "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." is consistent with how BP is used in practice in mathematical analysis of fluid dynamics. Granted, it's a calculational shortcut that does not precisely model the actual physical world. But it's close enough for engineering work. Note that the section is about "simplified explanations" and is not the proper place for a long technical discussion of exactly when BP applies and when it doesn't. ] (]) 03:28, 24 August 2021 (UTC)
"All attempts to fly in heavier-than-air machines must embody some means of forcing the air downwards so as to provide the equal and opposite reaction which is to lift the weight of the machine."


{{od}}{{ping|PrimalBlueWolf}} As you can see, I have moved your posts and the responses from me and {{ping|Mr swordfish}} to their own thread under this new heading.
"...if we reject the idea of flapping wings, we must replace it by some other device which will deflect the air downwards."


You have written “That is only valid along a streamline, …” That is incorrect in the case of a wing generating lift in the atmosphere. Consider the following:
''Mechanics of flight''<br>
Kermode, A.C.<br>
Eighth (metric) edition, 1972.<br>
Pitman Publishing <br>


In '''Fluid Mechanics''' by V.L. Streeter (1951 McGraw-Hill), section 3.7 ''The Bernoulli Equation'' says:
<hr>
<blockquote>The constant of integration (called the Bernoulli constant) in general varies from one streamline to another but remains constant along a streamline in steady, frictionless, incompressible flow. These four assumptions are needed and must be kept in mind when applying this equation.
Under special conditions each of the four assumptions underlying Bernoulli's equation may be waived.
1. When all streamlines originate from a reservoir, where the energy content is everywhere the same, the constant of integration does not change from one streamline to another and … may be selected arbitrarily, i.e. not necessarily on the same streamline.</blockquote>


In '''Aerodynamics''' by L.J. Clancy (1975 Pitman Publishing) section 3.4 ''Bernoulli's Theorem for Incompressible Flow'' says:
Reference added by ] (]) 21:08, 16 December 2014 (UTC):
<blockquote>Further, at some distance upstream of the aircraft, the flow consists of a uniform stream. It follows that on any given streamline in this region the value of p + 1/2 ρ v<sup>2</sup> is the same as it is on any other streamline.</blockquote>


In '''Fundamentals of Aerodynamics''' by John D. Anderson (1984 McGraw-Hill) section 3.2 ''Bernoulli's Equation'' says:
Elements of Practical Aerodynamics
<blockquote>For a general, rotational flow, the value of the will change from one streamline to the next. However, if the flow is irrotational, then Bernoulli's equation holds between any two points in the flow, not necessarily just on the same streamline.</blockquote>
Jones, B. 1939
John Wiley and Sons, Inc.


In the language of fluid dynamics we say Bernoulli's principle applies equally at all points on all streamlines in a region of ]. A wing operates in a stationary atmosphere so there are no viscous forces or vorticity in the air outside the boundary layers. The flow around a wing is irrotational everywhere except in the boundary layers.
In the context of an analysis of induced drag on p. 82 he makes the following statement about the downward momentum imparted to "the mass of air affected by the wing":


You have also written “… only accurate along a streamline where no heat is being transferred between the wing and the air.” I assume you are referring to transonic and supersonic flow. The Misplaced Pages article presently only refers to lift in subsonic flight. In low-speed flight there is no significant amount of heat being transferred. ] ''(])'' 04:32, 24 August 2021 (UTC)
"It has been proven mathematically that the downward momentum in unit time is equal to one-half the lift".


I'm glad to take the correction and agree with the reasoning. Thanks for the detailed and well sourced explanation. ] (]) 07:19, 24 August 2021 (UTC)
<hr>


== Proposed new version of simplified explanation continued ==
Section added by ] (]) 21:08, 16 December 2014 (UTC):


The last thread had gotten rather long, so starting a new one.
On the popular qualitative flow-deflection explanation based on Newton's laws:


Latest version now available in my sandbox.https://en.wikipedia.org/User:Mr_swordfish/sandbox
"The main fact of heavier-than-air flight is this: ''the wing keeps the airplane up by pushing the air down''.


I opted to keep the opening section, at least for now, but as it stands now there is substantial repetition between it and the first paragraph of the next section. Not sure what is the best solution, but I'm out of time for the day. Comments and suggestions appreciated. ] (]) 15:33, 26 August 2021 (UTC)
Stick and Rudder - An Explanation of the Art of Flying.
Langewiesche, W.
McGraw-Hill Education


:I spent some time today looking at other Misplaced Pages articles on technical, mathematical, or scientific subjects. I came away with two observations:


#The articles discuss the topic at hand, rather than discussing the article and how it covers the topic.
"In momentum-based explanations, it is generally argued that the airfoil produces a flowfield in which some of the air is "deflected" downward and thus has downward momentum imparted to it. To acquire downward momentum, the air must have a downward force exerted on it by the airfoil, and thus, by Newton's third law, the airfoil must have an upward force exerted on it by the air."
#None of them have language that implies that the topic is difficult to explain or to understand.


:With that in mind, the opening section "Understanding lift as a physical phenomena" would be an outlier in terms of Misplaced Pages style. The more matter-of-fact treatment in the section that follows is in keeping with wider Misplaced Pages standards.
''Understanding Aerodynamics -- Arguing from the Real Physics'' sec 7.3.1.7
McLean, D.
Chichester, West Sussex, U.K. : Wiley, 2013.


:See ], ], ], ], ], ], ] for a few examples.
<hr>


:On that basis I'm going to remove the section from the draft while repurposing some of the language into the new first section. At this point, I think we have a release candidate. Comments? ] (]) 15:31, 27 August 2021 (UTC)
Section added by ]


::I agree. I encourage you to release the latest version. ] ''(])'' 13:35, 28 August 2021 (UTC)
On the Newtonian theory of lift
:::It's been released. Thanks to everyone who contributed. ] (]) 21:06, 28 August 2021 (UTC)


Sorry for not weighing in sooner on the latest changes. I've been away for a few days.
"The fluid itself is postulated as a collection of individual particles that impact directly on the surface of the body, subsequently giving up their components of momentum normal to the surface, and then traveling downstream tangentially along the body surface. That fluid model was simply a hypothesis on the part of Newton; it did not accurately model the action of a real fluid, as Newton readily acknowledged. However, consistent with that mathematical model, buried deep in the proof of Proposition 34 is the result that the force exerted by the fluid on a segment of a curved surface is proportional to sin^2 (theta), where theta is the angle between the tangent to the surface and the free-stream direction. That result, when applied to a flat surface (e.g. a flat plate) oriented at an angle of attack alpha to the free stream, gives the resultant aerodynamic force on the plate:


I see that the proposed new section has been removed again and that some of the language has been "repurposed" into the following section. It seems to me that these changes have negatively impacted the article's organizational clarity. The first mention of the mathematical theories now comes under the heading "Simplified explanations.....", and with this placement the mathematical theories are now categorized as one of "several ways to explain how an airfoil generates lift". This isn't an accurate reflection of where the mathematical theories fit in the overall picture. The mathematical theories are the basis of the rigorous scientific understanding of lift. They're not "explanations" of lift.
R = rho*V^2*sin^2(alpha)


I think the proposed new section reflected the facts of the matter more clearly. Except for the phrase (referring to the simplified explanations) "and most readers will likely already have been exposed to one or more of them", which I propose we delete, everything that remains is a straightforward statement of fact. Even the one bit of "meta" information ("These issues are discussed in connection...") is a factual statement that more detail on the issues just raised is coming later in the article, not a "discussion" of "how the article covers the topic".
This equation is called Newton's sine squared law...."


I don't think that providing a bit of factual meta information is out of place in a Misplaced Pages article. Nor is it out of place to say that a correct qualitative explanation of lift is difficult, given that it's a statement of fact supported by the checkered history of qualitative explanations and by the sources (my TPT paper, at least).
A History of Aerodynamics
Anderson, J. D. , Jr.
Cambridge University Press


I've tweaked the proposed new section and removed its heading, which makes it part of the "Overview" section, where I think it fits well. I've also taken a crack at removing the resulting duplication from the intro to "Simplified physical explanations..." in my sandbox. My recommendation is to merge these changes into the article in place of the recently released version. ] (]) 19:27, 2 September 2021 (UTC)
<hr>


:Thanks for your continued effort on this page. I've made an attempt to merge your latest version with the current article. It's in my sandbox. https://en.wikipedia.org/User:Mr_swordfish/sandbox#Overview Comments appreciated. ] (]) 20:12, 4 September 2021 (UTC)
(work in progress - to be continued)
I'll try to track down the cites provided by Doug McLean and see if I can pull out the relevant direct quotes instead of relying on his summaries. Not that I don't believe his summaries, it's just that we'd be remiss as editors if we just took his word for it.
] (]) 21:33, 8 December 2014 (UTC)


::Mr Swordfish: I have no objection to the current version in your sandbox being released. ] ''(])'' 12:52, 6 September 2021 (UTC)
===Comments on the sources above===
Please make any comments below here, so that we can keep the listing of sources clean and uncluttered.


:::Mr Swordfish: Your rendition of the addition to "Background" is more cryptic than my draft, but I'm on board with all of it except the last sentence, which seems to me to be ambiguous. Actually, I think all, not just some, of the simplified explanations we present have the flaw of leaving important things unexplained, even the ones that also have incorrect elements. A possible revision:
*'''Comments on Prandtl and Tietjens'''
"...the integrated rate of change of vertical momentum for the atmosphere as a whole must be zero." Thus for the most obvious assumption a reader is likely to make regarding what is meant by "the air" (i.e. the atmosphere as a whole), The Original Statement is false. - DougMcLean (from earlier)


::::There are also many simplified explanations, but all leave significant parts of the phenomenon unexplained, while some also have elements that are simply incorrect.
*'''Comments on Durand'''
It is explicitly stated that this result holds regardless of how large the radius of the circle is made. Thus a large circle is another example of a region of "the air" for which a reader might reasonably expect The Original Statement to apply, but for which it is in fact false. - DougMcLean (from earlier)


:::I think we're almost done and on the verge of completing a significant improvement of the article. ] (]) 00:54, 7 September 2021 (UTC)
*'''Comments on Lissaman'''
::::I have implemented the suggested change in my sandbox and will deploy that version. However, I failed to start with the latest version from the real article and several changes have been made since I deployed the version from my sandbox so I can't just do a cut and paste or it will override those changes. So, there will be several intermediate versions in my sandbox as I reconcile the two. ] (]) 13:46, 8 September 2021 (UTC)
According to Lissaman's results, if "the air" is taken to be the air in a rectangular box surrounding the airfoil, The Original Statement isn't even close to being true unless the box is a tall, slender sliver, and even then it isn't strictly true until the vertical dimension of the box is taken to infinity. Steelpillow quotes the section of my book that describes the result for the infinitely tall, slender sliver, the only control-volume shape for which The Original Statement has been shown to be true, and interprets it as being "in support of The Statement". A balanced recounting of what my book says would also quote the discussion in connection with figure 8.5.4, which deals with other control-volume shapes for which The Original Statement isn't true. - DougMcLean (from earlier)


== Coandă effect criticism ==
*'''Comments on the AAPT paper'''


The following sentence was recently added:
The quote from the AAPT textbook committee given above is the ''entire'' discussion of lift in that paper. The paper itself is a 25 pager devoted to reviewing seven high school physics textbooks, and that's all the space they had to address lift. As such it is quite cursory and lacks context. They suggest seeing Waltham's paper for more details and context. Waltham in turn cautions that to do it "correctly" requires a control volume of infinite thickness.


:A criticism of the Coandă effect as an explanation for aerodynamic lift is that the Coandă effect itself is not well understood.
The AAPT does not explicitly say dp/dt of the entire atmosphere (or the "local flow" for that matter) is equal to -L. By not defining what they mean by "the air" they leave an imprecise statement that can be interpreted in different ways, one of which is correct and most of which are incorrect. If we repeat it with the same imprecision it is likely that our readers will latch on to one of the incorrect interpretations.


With a cite to https://digitalcommons.usu.edu/cgi/viewcontent.cgi?article=1096&context=etd
In sum, I would not give it the same ] as other more in-depth treatments of momentum transfer. ] (]) 21:09, 10 December 2014 (UTC)


The relevant part of that paper says:
The AAPT describe how much momentum is imparted to air within the atmosphere per unit time, consistent with results obtained by Lanchester, Lissaman and others.


<blockquote>The Coanda effect has been widely used in the both aeronautics and medical applications , air moving technology, and other fields. Nevertheless, this phenomenon is not completely understood, especially for three-dimensional flow as in the CSM design. The nature of the Coanda effect, with boundary layer separation and entrainment interaction, make for difficulty in solving the flow numerically and analytically.</blockquote>
I find it hard to think of a better form of words to describe this rate simply and concisely without going into details of a mathematical proof. ] (]) 09:20, 16 December 2014 (UTC)


I'm not seeing where the source ''criticizes'' the usage of the Coandă effect to explain lift, so this material appears to be ]. A bigger problem is that saying that "the Coandă effect itself is not well understood" is a very broad statement that would need stronger backing than the carefully worded excerpt from the cited Masters Thesis above. Reading the ] article I don't see anything supporting the assertion that it is not well understood - were this truly the case I would expect it to be treated in that article.
I agree with ] that the AAPT paper doesn't deserve "the same ] as other more in-depth treatments of momentum transfer", and that "to describe this rate simply and concisely without going into details" would be misleading. ] (]) 21:08, 16 December 2014 (UTC)


Of course, that wikipedia article is not dispositive - we're supposed to look at reliable sources, and other wikipedia articles are not reliable sources - but it strikes me that if we're going to publish a broad assertion like that the proper venue for discussing it and presenting the source material would be the talk page for that article, not this one.
*'''Comments on Lanchester'''
Lanchester §112 says that it is generally possible to show that dp/dt = -L. He goes on to clarify the exception commonly known as ]. ] (]) 10:13, 11 December 2014 (UTC)


I'm removing the material pending the production of better citations. ] (]) 20:32, 9 March 2022 (UTC)
Without the use of calculus, he derives the total directly from Newton's laws.


:I agree with Mr. Swordfish that better citations are necessary. However, as far as I have been able to determine, there are no sources that offer a well thought out explanation for why or how the Coandă effect applies to aerodynamic lift. The popular references quoted in the main article (references 33 and 34) certainly do not offer that explanation. This lack of a source making a detailed argument for applying the Coandă effect to aerodynamic lift is not apparent in the main article. I tried to make this deficit of a source argument, not vey well I must agree, but one that should be made. It is difficult to make this argument since there are no referenceable sources that point out this deficit of a source offering a valid explanation. ] (]) 16:51, 10 March 2022 (UTC)
The pressure ''w'' is entirely accounted for on the surface of the earth. ] (]) 07:20, 13 December 2014 (UTC)
::Were I writing this article for myself, I'd include something like:
:::People often try to explain why the air is deflected on the top of the wing by saying it's because of the Coandă effect, but this doesn't actually ''explain'' anything, it just gives it a fancy European name.
::But I'm not allowed to just make stuff up on my own and I haven't seen this idea expressed elsewhere so I don't have a source for it. And that means I can't add it to the article. That said, I agree with the sentiment that it's poor pedagogy to explain something via material that the reader doesn't understand either. And I think the article would be improved with a short statement like the one above or something similar to what you added, but unless we can find reliable sources to cite we can't add it. If you find a good source for this I'm all ears. ] (]) 23:23, 10 March 2022 (UTC)
Anderson and Eberhardt's "Understanding Flight" (McGraw-Hill, 1st ed. 2001) is the one source I know of that appeals to the Coanda effect in a lift explanation and also tries to explain how Coanda works in physical terms. They attribute the Coanda effect entirely to viscous "shear forces." On p. 23, after explaining no-slip at the surface and the resulting formation of a boundary layer, they say:
:"The differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer. This causes the fluid to try to wrap around the object."
This explanation of Coanda is easy to rebut. However, my own book ("Understanding Aerodynamics", Wiley, 2012) is the only citable source I know of that does so explicitly. With reference to using Coanda in lift explanations, I say in sec 7.3.1.7:
:"The Coanda effect is erroneously seen as implying that viscosity plays a direct role in the ability of a flow to follow a curved surface. Anderson and Eberhardt assert that viscous forces in the boundary layer tend to make the flow turn toward the surface, specifically, as they put it, that the 'differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer.' Actually, there is no basis in the physics for any direct relationship between shear forces and the tendency of the flow to follow a curved path."
In the paragraphs following the above, I explain in detail my reasons supporting the statement in that last sentence. The gist of it is that the curving of the flow is a result of the interaction between the pressure field and the velocity field, as we explain in the article under "A more comprehensive explanation." It has practically nothing to do with viscous or turbulent shear stresses. As long as the boundary-layer doesn't separate, the curving of the flow to follow the curved surface is an essentially inviscid effect.


] has invited us to identify a citable source for his naming-isn't-explaining objection to relying on Coanda. Again, the only one I know of is my own book. In sec 7.3.2 I list things to avoid in an explanation of lift. Item 5 is:
:Lanchester's §112 does not say "that it is generally possible to show that dp/dt = -L." His analysis only shows that it is possible if you make one particular assumption for the shape of the control volume.
:"'Naming' as a substitute for explaining, as, for example, in saying that a jet flow follows a curved surface because of the Coanda effect, where 'Coanda effect' is just a name for the tendency of jet flows to follow curved surfaces."
So we have citable sources for a couple of possible additions to the Coanda subsection that would be of interest to some readers. I'm not enthusiastic about doing it, however, because I think we may already be giving Coanda more prominence than it deserves. On the other hand, I could argue that the article as it stands doesn't present enough of the case against Coanda, and that the additions we're considering here would balance things better and help justify the word "Controversy" in the article's section heading.] (]) 20:20, 3 April 2022 (UTC)


:Thanks very much Doug. {{u|Mr swordfish}} and I will ensure your book is cited as a source where it is appropriate to do so in relation to Coanda effect. ] ''(])'' 23:49, 3 April 2022 (UTC)
:Lanchester's §112 amounts to a verbal version of a control-volume analysis for a tall-sliver control volume in contact with the ground. Lissaman (1996) published the corresponding analysis for the free-air case. The result is the same whether there is a ground plane or not, i.e. that as the height of the sliver goes to infinity the pressure force at the bottom (and top in the free-air case) vanishes, and thus dp/dt = -L for a control volume that is infinitely tall compared to its width.
::Now that we have a cite I've been trying to craft language along these lines, but so far haven't come up with anything that doesn't seem out of place or unencyclopedic. I'll keep trying. Suggestions cheerfully considered. ] (]) 23:56, 11 April 2022 (UTC)
:::{{u|Mr swordfish}} and {{u|J Doug McLean}} I have inserted a paragraph that, hopefully, begins to capture some of Doug's wisdom from above. See my . ] ''(])'' 04:41, 27 September 2022 (UTC)
::::I have also added a sentence on "naming is not explaining". ] (]) 18:55, 28 September 2022 (UTC)


== A new simplified lift explanation ==
:Lanchester's result is essentially the same as Lissaman's and doesn't support an unapologetic version of The Statement any more than Lissaman did. The pressure is "entirely accounted for", but it's effect vanishes only because the height of the sliver is taken to infinity and the width is kept finite. ] (]) 21:08, 16 December 2014 (UTC)


As if things weren't complicated enough, I have developed a new simplified explanation for aerodynamic lift that I would propose as a add-on to the present version. I am looking for comments and recommendations at this point.
::{{talkquote|Lanchester's §112 does not say "that it is generally possible to show that dp/dt {{=}} -L."|J Doug McLean}}


The proposed text is available in my sandbox at https://en.wikipedia.org/User:David_Weyburne/sandbox
::Yes it does. Providing the right physical conditions exist, it is always possible to make the assumptions which show dp/dt is practically equal to -L. Lanchester suggests that when an aerofoil is in ground effect, w may become significant, in which case it would not be possible to show dp/dt = -L. He characterises the former situation as "ordinary conditions" which would "ususally be the case".


The proposed explanation is based on a graphical interpretation of the mathematical equations governing fluid flow. The key to the approach is the graphical plots of the velocity profiles and the pressure gradient profiles taken at a bunch of locations along the airfoil surface. This permits a one-to-one correspondence between the flow governing equations and the plotted profiles. By invoking the momentum conservation equation in this way, the explanation provides the connection between the velocity and pressure fields that is missing in the other simple explanations. ] (]) 13:38, 17 September 2022 (UTC)
::I only mentioned the fact that Lanchester accounts for pressure on the surface of the earth in response to your previous suggesting Lanchester supports your argument against The Statement.


:Where a Misplaced Pages User develops a new explanation for something it is called Original Research. Such an explanation is not published in Misplaced Pages - see ].
::It is clear from previous discussion and your obvious expertise in the subject that you need no explanation of the physics. So it is a mystery to me why you repeatedly misrepresent what has been written by others. You jest that is "part of the fun of being an aerodynamicist". I have not made a mistake here. We are ] for an exercise in schadenfreude.
:Your explanation cannot be described as simplified. I find it mystifying. Some of your sentences are statements of the obvious and therefore unnecessary in your description; and others are either incorrect or misleading. If you wish to continue with your work on this subject in order to publish it in an appropriate place, it needs a lot of refinement.
:You are relying on four sources but three have been published by yourself. This is usually unwise and I have commented at ]. ] ''(])'' 23:20, 17 September 2022 (UTC)
::Thanks for the feedback. As to original research comment: I do not think any of the explanations presented in the Simplified Explanations section would constitute original research that would be appropriate for a journal article. The explanation may be original but it is not something that can be tested and verified by other research groups. As to the rest of the comment: I am sorry you find it mystifying but I am hoping that is not the case for the majority of readers. You claim there are obvious statements that are unnecessary: I have tried to make the explanation readable for the non-expert and would hope that the expert reader would allow for that. You also claim there are misleading and incorrect statements: It is hard to comment on this claim since you did not bother to outline which statements are false or misleading. ] (]) 12:54, 21 September 2022 (UTC)


:::{{u|David Weyburne}} Thanks David. On 18 September I made some introductory comments about statements I regard as superfluous, and others I regard as misleading. Those comments are on one of your Talk pages - see ]. ] ''(])'' 23:05, 21 September 2022 (UTC)
::I've no doubt that that Lanchester's §112 is essentially the same as Lissaman's result. Both show that momentum is imparted to air within the atmosphere at a rate equal to lift. I don't see anything misleading about describing this rate as a simple fact in an introductory text, as advocated by the AAPT. You may disagree, but they are experts at educating people. ] (]) 12:07, 17 December 2014 (UTC)
:::Sorry, I initially missed your comments in my sandbox. I appreciate your detailed comments and I have replied to the comments in the Talk section. At this point I will leave the explanation as is and would add that a more detailed explanation is available in the supplied references. ] (]) 12:40, 22 September 2022 (UTC)
::One further note as to the observation that three of the sources were published by myself and is therefore inappropriate. I would point out that one is a YouTube video, another is an Air Force Technical Report, and the third is an e-book collection of my Air Force Tech Reports. All of them lay out a more detailed version of the condensed simplified explanation provided in my Sandbox. The reason the references are all mine is that I believe that my simplified explanation is original. However, as I stated before, this type of simplified explanation is not something that would be appropriate to be published in a standard journal. It is appropriate for providing a simplified explanation in an encyclopedia-style format. ] (]) 12:45, 23 September 2022 (UTC)
:::As the author of the proposed cited articles you may be subject to ]. I would suggest familiarizing yourself with that policy. I appreciate the fact that you have disclosed that you are the author of those articles, but that fact remains and is germane and therefore not inappropriate.
:::That said, the fact that the proposed additional material uses your articles as their source doesn't mean that the material can't be added to the article, or that your articles can't be cited. We've encountered this issue before with a prominent author, who provided some very valuable insights into this topic and helped improve the article. But he made very few edits himself, instead working with the other editors to reach consensus about any proposed revision to the article. I think we are on solid grounds if we follow that model. ] (]) 19:38, 23 September 2022 (UTC)
::::Sorry, been busy. I understand that referencing my own work is problematic. To explain the reason for doing this, I need to give a little background. My simplified explanation for aerodynamic lift is based on showing "graphically" how the conservation of mass, momentum, and energy occurs for a flow around an airfoil. To do this, I start using a simple word-based argument to say that mass diversion results in velocity changes while being diverted around an airfoil. These velocity changes result in a speed up for the flow on the airfoil. How do you graphically show this speed-up? It is possible to use streamline, contour, or vector plots of the velocity but because of the large spatial variations, this approach is not very effective. Hence, most simplified explanations for lift regress to simply stating that "the velocity speeds up". For my simplified explanation I switched to a series of "velocity profile plots" along the airfoil. The profiles show the velocity behavior from a point on the airfoil to a point deep in the free stream above the airfoil. What you see are velocity peaks near the airfoil surface that slowly return to the free stream over distances of ~two chords. These peaks are important in that it gives a visual confirmation of velocity changes and give a one-to-one comparison to the momentum equation du/dy term. The momentum equation says these velocity changes must be conserved which is done, in part, by pressure changes. I then can show a plot of the pressure gradient profiles above and below the wing at the same location as the velocity profiles. The difference in the pressure profile areas, the pressure difference, shows graphically how mass and momentum conservation results in lift.
::::So what is the problem, why do I only reference my own work? The reason is there is no one doing anything similar using velocity profiles. This velocity profile "peaking" behavior is not discussed or plotted anywhere in the literature that I could find (other than the simple text saying "the velocity speeds up"). Many textbooks show schematics of boundary layer profiles but not ones that show the peaks, the velocity speedup behavior. I observe it my airfoil simulations and in raw mesh data provided by other researchers, but nowhere in the literature. If I had references showing that these velocity and pressure profile peaks exist, I would be less dependent on referencing my own work. For the record, I think for the non-expert, my 15 min. graphics-based YouTube video does a better job of explaining this aerodynamic lift argument than my e-book version.
::::I would be willing to work with any editor to resolve this issue. ] (]) 15:03, 23 March 2023 (UTC)


== Recent changes to equal transit time section ==
:::What I've said repeatedly is that the only published sources that use a realistic flow model and find dp/dt = -L to be true are those using a very-tall-sliver control volume. These sources make no claim that dp/dt = -L is true in any more general sense than that. So what, specifically, have I misrepresented?


The diff is here: https://en.wikipedia.org/search/?title=Lift_%28force%29&diff=1228641725&oldid=1227711027
:::You still seem to have concluded that The Statement is somehow true in a more general way. To me, this doesn't seem consistent with the physics or the published evidence. Just because dp/dt = -L applies in one particular control volume doesn't mean it applies to "the atmosphere" in any general sense. Yes, the tall sliver control volume "exists within" the atmosphere, but so do other control volumes for which dp/dt is different from -L. I see no basis for thinking one control volume is the "correct" one and the others are not. In general, the force exerted on the air by the foil is manifested as a combination of momentum changes and pressure differences in the flowfield. The one control volume for which the integrated pressure differences happen to vanish isn't in any fundamental way more "correct" than the others.


I don't read the previous version as claiming that equal transit time never happens, only that it cannot be assumed. The "offending" passage is:
:::I know of no published source that uses a realistic flow model and shows that dp/dt = -L is true in the general sense you're proposing. The AAPT paper presents no analysis, and Chris Waltham's paper doesn't count on this score because he uses a simplified flow model that omits the crucial effect of the pressure field, as discussed in my comments on Clancy.

:This is because the assumption of equal transit time is wrong. There is no physical principle that requires equal transit time and experimental results show that this assumption is false.
:::No, the Statement is not a "simple fact". It is a statement that is misleading unless it is accompanied by a somewhat arcane caveat. And I'm not making these arguments for fun. I'm here to improve the article by avoiding the inclusion of a misleading statement. ] (]) 22:52, 19 December 2014 (UTC)

::::In answer to your question, I have already clarified why I said, "Lanchester §112 says that it is generally possible to show that dp/dt = -L. He goes on to clarify the exception commonly known as ground effect." My comment is supported by the citation above. Your contradiction takes my words out of context.

::::The earlier comment I referred to said, {{talkquote|Actually, Lanchester's "deficiencies" section provides no support for The Statement, but instead supports what I've been arguing all along. The "Newtonian medium" (a hail of projectiles that don't interact with each other) is a poor model for flows of real fluids.|J Doug McLean}} This is a rebuttal for a proposition that was never made. The point of discussion was whether or not The Statement is true.

::::Several sources clearly explain how to calculate the result dp/dt = -L. As I have explained repeatedly, all of them account only for momentum. There are other calculations which account partly for pressure differences and for a smaller proportion of momentum. Your repeated assertion that other results for dp/dt are different, yet somehow answer the same question defies common sense. Again it is a rebuttal for a proposition that the cited authors did not make.

::::I'm afraid this is going round in circles again. Hopefully in the New Year there will be some progress on improving the article. ] (]) 12:26, 20 December 2014 (UTC)

*'''Comments on Clancy'''
It is interesting that Clancy sees no contradiction between his Newtonian description and the fact that at the trailing edge, only half the momentum has yet been transferred. &mdash; Cheers, ] (]) 09:51, 15 December 2014 (UTC)

As far as I can tell, in the idealised infinite situation he goes on to describe Clancy is arguing that although the downward change of momentum in any finite portion of air is now infinitesimal, the sum of infinitely many such portions remains finite and is in fact still equal to the reaction to the lift. &mdash; Cheers, ] (]) 16:11, 11 December 2014 (UTC)

Clancy refers to "the affected air". This compares to the phrase "the air" which has caused so much supposed scope for misunderstanding here. Simply inserting the word "affected" as Clancy does would clear that side issue up. &mdash; Cheers, ] (]) 09:36, 12 December 2014 (UTC)

:I don't think inserting the word "affected" will solve much of anything. According to the model, the entire atmosphere is affected by the presence of the moving airfoil so the "affected air" is all of it. And we have seen that for the entire atmosphere dp/dt =0. A few months ago we tried inserting "the air deflected by the foil" and that didn't do it either. There is some subset of the air for which dp/dt=-L, but I'm at a loss for how to state this in layman's terms without it being so awkward and convoluted that it distracts from the flow of the simple introductory section. ] (]) 13:10, 15 December 2014 (UTC)
::It is not true that, as you suggest, "According to the model, the entire atmosphere is affected by the presence of the moving airfoil." Nowhere does Clancy's model address the entire atmosphere. It addresses a certain cylinder of air which he first makes finite and then expands to infinite size. I wonder if you are confusing this infinite cylinder with the whole atmosphere? We can be sure that they are not the same thing because within the interior of Clancy's model infinite cylinder, dp/dt = F while we know that within the even more infinite atmosphere which contains his model, dp/dt = 0. "The affected air" in his model is just the air within the rear part of the cylinder, aka "the air deflected downwards". &mdash; Cheers, ] (]) 16:52, 15 December 2014 (UTC)

:::Apologies for not being clear, but I wasn't referring to Clancy's model - I was referring to solutions to the Navier-Stokes equations, Euler equations, potential flow , etc.

:::In the very simple case of potential flow, the resulting flow field is the superposition of a steady uniform flow (i.e. what the flow would be like in the absence of the foil) and a vortex flow. While the vortex flow field diminishes as one gets farther away from the foil, at least in theory it is non-zero everywhere. So in the potential flow model the entire atmosphere is affected by the foil. More rigorous models (N-S, CFD, etc) give similar non-zero deviations from uniform flow throughout the entire atmosphere. These mathematical treatments are what I meant by "the model".

:::It appears that when Clancy says "the air" he means some specific subset of the atmosphere which he has defined beforehand and not the entire atmosphere. Fair enough, but unless we provide such a definition to our readers it is likely that they will interpret "the air" as the entire atmosphere. I think we are in agreement that for a non-accelerated foil dp/dt of the entire atmosphere is zero. If so, we're just arguing over what is meant by "the air". If not, then our disagreement is more fundamental. Which is it? ] (]) 19:55, 15 December 2014 (UTC)
::::Ah, in an item headed "Comments on Clancy", I hope you will forgive my misunderstanding which model you were discussing. The sources certainly bear out that the overall dp/dt is zero, I have no problem with that. Perhaps the best approach to "the air" is simply to write the new section intelligibly and not worry about our past usage. My comment on Clancy's usage was really just a flag to that end, in case it came in useful. &mdash; Cheers, ] (]) 20:50, 15 December 2014 (UTC)

:::::Clancy himself admits that his flowfield model is "very crude". It assumes that "the air affected" by the wing in 3D is limited to a stream of circular cross-section with diameter equal to the wingspan (fig 5.21) and that this air is uniformly deflected downward by its interaction with the wing. There is no upward turning ahead of the wing or behind as there is in more-realistic flow models.

:::::His model is unrealistic in another respect, and that is that it completely neglects the pressure field. It is assumed that the only force acting on the affected stream is that exerted on it by the wing, and this force is assumed to show up entirely as a rate of change of momentum of the steam of affected air. Thus dp/dt = -L is not really a result of this analysis; it is more of an a priori assumption.

:::::His model becomes a little less unrealistic in 2D, where the wingspan and the diameter of the affected cylinder have gone to infinity, and the entire flow is thus affected, but it is still unrealistic in assuming the flow deflection is uniform, and in neglecting the pressure field.

:::::Both Durand and Batchelor rigorously show that a uniform flow plus a vortex is a good approximation for the far-field flow in 2D, regardless of the details of the airfoil shape. The classical control-volume analyses I've cited use this model and show that the pressure field exerts significant forces on "the air" except in the case of the infinitely tall sliver.

:::::I would not give Clancy the same weight as I would to the classical analyses I've cited, which use a much more realistic model. And I agree with ] that adding "affected" doesn't clear up what is meant by "the air". ] (]) 21:08, 16 December 2014 (UTC)
::::::I am quite sure that you would give your own work more weight than you give to those whom you criticise. Yawn. Worse, you cherry-pick from Clancy's full text to support your PoV. It also notes that his simplified model is consistent with a more complex analysis he gives later - and when we turn to that later analysis we find that it embraces the very flow-plus-vortex model you approve of. To selectively quote and then claim that Clancy's simplified model is at odds with the flow-plus-vortex model is somewhat invidious. Turning to the classical analyses you have quoted from, we may note that Clancy also writes that the downwash at the trailing edge is only half of its ultimate value, which it achieves a little over a chord-length further downstream. This is entirely supported by the classical analyses you quote. If I had had a different textbook on my shelf introducing these standard results using the standard introductory model, I am sure you would have laid into them equally. To claim that a standard textbook such as Clancy is at odds with the mainstream is to seriously undermine your own position. &mdash; Cheers, ] (]) 11:02, 17 December 2014 (UTC)

:::::::All of the quotes attributed to Clancy in the "sources" section above are from chapter 5, and all are based on the simplified flow model he uses there. In criticizing this model, I am not "cherry-picking". I'm sticking to the topic under discussion, i.e. the weight these different sources should be given regarding the question of dp/dt in the flow around a lifting foil.

:::::::You say that his results from chapter 5 are "consistent" with his results from the more realistic model in chapter 8. That's simply not true with regard to the question we're discussing here. The issue of dp/dt isn't addressed at all in chapter 8. The only part of the book that deals with dp/dt due to lift is chapter 5. So to criticize the model he uses in chapter 5 is not to "selectively quote" him.

:::::::The only thing for which Clancy claims the two models yield equivalent results is in the variation of the downwash from the near field to the far field, which does not address the question we're discussing here. The downwash velocity is a local quantity, while the dp/dt we're discussing is an integrated quantity.

:::::::In chapter 8 he uses the horseshoe-vortex model for a 3D wing, for which it is said that both the bound vortex and the trailing vortices contribute to the downwash field. But when he says that the downwash in the near field is only half the value in the far field, he's changed gears and he's referring only to the "3D" part of the downwash, the part associated with the trailing vortex system, and omitting the part of the downwash associated with the bound vorticity. I mention these details only to rebut your claim that "This is entirely supported by the classical analyses you quote." No, the analyses I quote deal with integrated dp/dt in a control volume, not with the variation of the downwash velocity downstream. And all but one of them deal with the 2D case, where the downwash velocity doesn't behave at all as Clancy describes for the 3D case anyway.

:::::::I'm not criticizing Clancy's book as a whole. I'm criticizing the applicability of the model he uses in chapter 5, and the statements he derives from it, to the question of dp/dt. And yes, I do find that in neglecting the pressure field he's at odds with the mainstream analyses on this particular issue. If you have any actual specific counterarguments to make in this regard, please let us know what they are. ] (]) 22:52, 19 December 2014 (UTC)

*'''Comments on Chris Waltham's ''Flight without Bernoulli'' '''

In the section titled "A Simple Model", Waltham uses the same kind ot model Clancy uses in sec 5.15, i.e. the model in which the air is affected only within a stream of limited cross-section. He starts with the assumption that the cross-section is rectangular, but he later says that it could just as well be circular. This model is unrealistic for the same reasons I give in my comments on Clancy. Because the model does not represent the flow realistically, it is wrong on some important details, such as dp/dt in the local flow around the wing. Regarding the question of dp/dt, I would not give Waltham the same weight as I would to the classical sources. ] (]) 21:08, 16 December 2014 (UTC)

*'''Comments on the popular qualitative flow-deflection explanation based on Newton's laws'''

I have added new section to the sources list: "On the popular qualitative flow-deflection explanation based on Newton's laws". It lists only two sources so far, but more can be found on NASA websites and elsewhere.

I think this kind of thing is the appropriate level of detail for the "Flow deflection and Newton's laws" section, and that we should not include a quantitative dp/dt statement there. ] (]) 21:08, 16 December 2014 (UTC)

*'''Comments on the "Newtonian" approach'''

In the "Sources" section I've added a quote from J. D. Anderson describing Newton's theory of lift, based on modeling the flow as a hail of bullets. The flow models used by Clancy and by Chris Waltham are similar to Newton's model in the sense that they assume that only a limited portion of the flow interacts with the foil, and they take no account of a continuum pressure field. Like Newton's theory, these "fire-hose" models are wrong about important details of the flow, such as dp/dt in the near field. As I argue above, Clancy and Waltham should be given less weight as sources on the topic of dp/dt than the classical sources that use a more realistic model. ] (]) 20:03, 20 December 2014 (UTC)

== Some diagrams to help clarify the discussion of 'The Statement' ==


We've created quite a wall of text arguing about ''the statement'', and don't seem to be getting anywhere. Perhaps some pictures can help clarify things.

Here's a diagram of an airfoil generating lift, with the airflow coming in from the left. Ahead of the airfoil in region A the air is accelerated upwards (upwash), in regions B and C the air is accelerated downward, and in region D the air is accelerated upwards as it returns to horizontal flow.

]

Let's say we ''define'' the regions accordingly, where A is the region in front of the foil where dp/dt>0 (upward acceleration) B and C are the regions above and below the foil where dp/dt<0, and D is the region behind where dp/dt>0.

When I encounter the phrase "the air deflected downwards" I parse that to mean the union of regions B and C. Perhaps there's some other interpretation that can be used, but that's what "the air deflected downwards" means to me. If there are other interpretations floating about I'd be happy to hear them.

What can we say about the net momentum transfer of B ∪ C? I do not know of any source that gives this value dp<sub>B∪C</sub>/dt. But we can infer how it relates to L by looking at the following sub-region of B ∪ C:

]

Region E is a tall thin sliver and if we take the limit of dp<sub>E</sub>/dt as the height goes to infinity <s>and the width goes to zero</s> we get dp<sub>E</sub>/dt = -L. Since this is a proper subset of B ∪ C and all of B ∪ C has negative dp/dt, E must have a lower magnitude of momentum change than all of B ∪ C. That is, for B ∪ C |dp/dt| > |L|. Earlier, Doug claimed to have calculated it to be -1.6L, which sounds plausible.

Now, I'm not suggesting that the above analysis (along with my crude diagrams) go into the article - it's certainly too arcane for the intro section and it's not ready for "prime time" as a later section. But I hope that my fellow editors can read it and understand why I have a problem with saying "the time rate of change of momentum of the air deflected downwards" is equal to the lift. By my interpretation of 'the air deflected downwards' the statement is incorrect. It took me a while to come around to this view - recall that I actually wrote ''the statement'' and included it in my re-draft last summer - but I now see that it's problematic. Comments? ] (]) 17:21, 22 December 2014 (UTC)
:I am having trouble following your summary:
:#The "width" which goes to zero is not defined - the width of what? Is it of the aerofoil chord or just of the column E, or perhaps the span orthogonal to the screen?
:#Whatever the "width" is, I find it hard to justify the statement that "as ... the width goes to zero we get dp<sub>E</sub>/dt = −L" (unless you are also implying that as the width goes to zero, L also tends to zero, which is not very helpful).
:If you believe what you wrote, then I can indeed understand why you have a problem with the Statement. But more fundamentally, I think you are still confusing a broad statement of the Newtonian principle with an attempt at detailed analysis. The Statement is expressing the Newtonian principle in a few words, while you are seeking to interpret some of those words ''ab initio'', i.e. without prior acceptance of the principle. That is bound to end in tears. &mdash; Cheers, ] (]) 14:51, 23 December 2014 (UTC)

::] presents a clear, detailed analysis of the problem with The Statement. There is one substantive problem with the analysis as presented, which ] has picked up on, and that is that it doesn't make sense for the width of column E to go to zero. But this problem doesn't invalidate ]'s conclusion.

::In his analysis of the tall sliver control volume, Lissaman took the limit as the height goes to infinity, but not as the width goes to zero. With an actual foil in the picture, a proper control-volume analysis of the lift requires that the control volume be wide enough to bracket the projected chord of the foil. I'm sorry if the word "sliver" confused the issue here. I used it to refer to the control volume's proportions, meaning to convey that the control-volume width is small compared to the height, not that it is small compared to the chord. Anyway, even though the width doesn't go to zero in Lissaman's analysis, the pressure difference between the top and bottom vanishes as the height goes to infinity, and the integrated vertical pressure force vanishes, with the result that dp/dt = -L, independent of the width, as long as the width is kept finite.

::For E to be a proper subset of B ∪ C, and to not include part of A ∪ B, the width of E must be restricted compared to what Lissaman assumed, with the vertical boundaries pushed up against the leading and trailing edges of the foil. But Lissaman's analysis still applies, and dp/dt = -L for E.

::]'s point 3 is mistaken. He says "E has a smaller magnitude which means that it is closer to zero and is therefore 'greater than' −L." No, E is the subset with dp/dt =-L, so its dp/dt cannot be "'greater than' −L.". ]'s analysis is correct.
:::Ah, yes, thank you for pointing that out. Too much Christmas spirit in my glass, I fear. I have now deleted that item. &mdash; Cheers, ] (]) 22:59, 23 December 2014 (UTC)
::] is also mistaken when he says "But more fundamentally, I think you are still confusing a broad statement of the Newtonian principle with an attempt at detailed analysis." No, dp/dt = -L for "the air" can be established as a valid "statement of the Newtonian principle" only after a detailed analysis has shown that -L is indeed the resultant force acting on "the air". And analysis has only shown this to be the case for the tall sliver control volume.

::]'s analysis above clearly shows that dp/dt = -L is false for "the air deflected downward". However, we have no citable source for this argument. On the other hand, even if we thought dp/dt = -L was true for "the air deflected downward", we have no citable source that supports including the word "deflected". To stay within what our sources support, our only choice is The Original Statement from the AAPT paper, without the word "deflected".

::I agree that The Original Statement in unapologetic form is unacceptably vague. If we include it in the intro section, we must, at a minimum, also specify that the only definition of "the air" for which it's been shown to be true is "a region that is very tall compared to its width", citing Lissaman. As I said long ago, I think the best option is not to make any quantitative statement in the intro section and to discuss the quantitative momentum balance in a new later section.

::I'd like to see something like ]'s ABCDE discussion in this new section, but I know of no citable source for it. From the sources I know of, I think the best we can do is to describe the results for the circular and rectangular (tall, square, and flat) control volumes in free air, and the atmosphere with a ground plane. Here are two possible diagrams I've made for the purpose, and I've started drafting candidate text to go with them.

]

]

::If we mention the "fire-hose" models at all (Clancy, Waltham), it would only be to point out their deficiencies relative to the more rigorous analyses. I'm proposing that it be a new subsection titled "Analyses of the integrated momentum balance in lifting flows", under "Mathematical theories of lift", just after "Circulation and the Kutta-Joukowski theorem". ] (]) 22:36, 23 December 2014 (UTC)
:::This is just the same old same old. The article is not going to be amended to support a view unsubstantiated by reliable sources. &mdash; Cheers, ] (]) 22:59, 23 December 2014 (UTC)

:::''There is one substantive problem with the analysis as presented ... it doesn't make sense for the width of column E to go to zero. '' Thanks. I have struck that language.

:::I look forward to seeing the draft section. Agree that anything we put into the article must have a citable source. ] (]) 00:46, 25 December 2014 (UTC)

:], I suggest you think about how ''dt'' should be handled in these calculations. You may find helpful.

: When making content decisions, we should be guided more by ] than by ]. The novel, unpublished analysis above will not help anyone understand the relevant physics. If you haven't already, I recommend reading Lanchester §112 for a straightforward explanation. ] (]) 14:58, 27 December 2014 (UTC)


::At this point I would like to ask both ] and ] to elaborate on what they think "the air deflected downward" means. I think we are in agreement that it doesn't mean the entire atmosphere since dp/dt of the entire atmosphere is zero. So, what does "the air" mean? I've given my interpretation and Doug has given several possible reasonable interpretations (of which only one makes ''the statement'' true). What's yours? And is it likely that our readers will have the same interpretation?

::Agree that we should value RS over OR discussion on the talk page, and I'll keep trying to chase down a copy of Lanchester and read sec 112. ] (]) 21:28, 27 December 2014 (UTC)
:::Since the Statement is just the application of Newton's laws to lift in words, in this context it means, "the air deflected downwards in reaction to the lift force." Not any other air deflected downwards because of some vortex or some distant pressure distribution or some clever analysis or whatnot. It is simply affirming that if we apply F=dp/dt to L, then there is a mass of air whose dp/dt is in reaction to L. Our clever analysis can then identify the location of this mass for us, and different analytical models will identify different locations (e.g. Clancy's firehose). Crucially, it is not saying that this is the only approach, nor even the best approach, just that it is an approach. Other models based on other approaches, say on pressure, will not even yield dp/dt=L because they have already accounted for much or all of L some other way. The sources can then indicate the due weight that each deserves. This is how pretty much every textbook treats it, and I am not aware of widespread misinterpretation among engineering students. I am confident that our readers will be no different. One can really only misinterpret it once one has gained a good deal of detailed knowledge, well beyond the introductory stage at which it is appropriate. &mdash; Cheers, ] (]) 22:10, 27 December 2014 (UTC)

:::Apologies for taking so long to reply.
:::I don't have any fundamental disagreement with your position. I do think Doug has a point (made elsewhere) that defining "the air" as the region that makes the statement true is somewhat circular, but the fact remains that there is such a region and I'm comfortable eliding over some of the details in the introductory section. To that end, I've prepared a draft in my user space that may help move us towards consensus. I'll introduce that in a new thread. ] (]) 19:56, 7 January 2015 (UTC)

==Suggested revisions==

I have posted a proposed revised version of the article in my sandbox ]. Changes from the current version are limited to two places:

:1) Under "Flow deflection and Newton's laws" I have removed the quantitative statement about momentum and done a bit of rewording of what remains to be sure that both the second and third laws still get their due.

:2) At the end of "Mathematical theories of lift" I have added two new subsections: "Analyses of the integrated momentum balance in lifting flows" and "Newtonian theories of lift".

Everything I've included has a citable source and is presented, I think, from a neutral point of view.

I think removal of The Statement is best for the following reasons:

:1) In this part of the article and at this level ("Simplified physical explanations..."), the flow deflection explanation is better off without it. This explanation is usually presented in its qualitative form anyway.

:2) Without the qualification that it's only been found to be true for the tall sliver, The Statement is open to misinterpretation. ] and ] still seem to think that it isn't, but I think their confidence that the typical reader will know how to interpret it correctly is unjustified. I think it's just too easy for an uninitiated reader to assume that "the air deflected downward" could refer to the atmosphere as a whole or at least to some sufficiently large subset of it. The atmosphere as a whole may be a "nonsensical" assumption as ] called it, but I wouldn't expect the typical reader to know that unless we tell him. And I certainly don't expect the typical reader to realize that it's true only for a particular shape of region.

:3) A general, unapologetic "dp/dt = -L" isn't consistent with what the mainstream literature says about dp/dt.

The two new sections are pretty self-explanatory. I included a paragraph on Newton's bullet model because I think it's interesting in its own right, it had an impact on early assessments of the practicality of heavier-than-air flight, and it helps put the "fire hose" models in perspective, which I also included under "Newtonian theories".

Looking forward to comments and suggestions.

] (]) 23:53, 30 December 2014 (UTC)

::First of all I would like to thank {{ping|J Doug McLean}} for all the hard work that has gone into this. The only real issue I have with any of it is the well-worn one we are all familiar with.
::Given all the quotations we so carefully collected above, quite how anyone can maintain that the mainstream sources do not support the momentum statement - and right at the introductory stage at that - is beyond me. Mainstream sources do include it, and even mandate it there. Ours is not to reason why or to sanitise it out of the article. It is there in the article, it is reliably cited, and there it must stay. Doug McLean makes some other minor textual changes to this section which are generally good.
::The bulk of the new section on "Analyses of the integrated momentum balance in lifting flows" is good, though there is a certain residual defensiveness in the last few sentences which can probably simply be omitted. Also, I would shorten the heading to just "Integrated momentum balance in lifting flows".
::The next section - the critique of the momentum model - is useful as far as it goes. However I think it needs a balancing critique of the other simple model we introduce, viz. the pressure model. These critiques could better introduce the whole section on "Mathematical theories of lift" rather than conclude it. Alternatively, they could be confined to their respective introductory subsections on "Limitations of ..." &mdash; Cheers, ] (]) 10:52, 31 December 2014 (UTC)

:::I agree with ] there is no justification for removing the existing momentum statement. I'm also grateful for progress on improving the article.

:::One minor point - I haven't been able to find Shapiro to reference the momentum equation, but I have found which says (in abbreviated terms):

:::'''F''' = d'''M'''/dt = '''F'''<sub>B</sub> + '''F'''<sub>S</sub>

:::I understand that in steady flow, '''F'''<sub>B</sub> = 0, so '''F''' = '''F'''<sub>S</sub>.

:::In ], I read the last two sentences of the first paragraph as '''F'''<sub>S</sub> = '''F'''<sub>B</sub>. Is this the intended meaning? ] (]) 18:06, 1 January 2015 (UTC)

:I have now incorporated what I believe to be the bulk of the proposal into the article, save for two parts: I retained the Statement along with its citations, and I have not copied across the subsection on Newtonian theories of lift because I am not yet sure where to put it. &mdash; Cheers, ] (]) 14:01, 4 January 2015 (UTC)

===Momentum theorem===
I still don't have an answer to my question above. A Google search for "momentum theorem for a control volume" brings back mainly references to ]. Is this what is being described? ] (]) 14:58, 4 January 2015 (UTC)
Here is an actual quote from Shapiro:
{{quotation|Eq. 1.13 is usually called the momentum theorem and states that the net force acting instantaneously on the fluid within the control volume is equal to the time rate of change of momentum within the control volume plus the excess of outgoing momentum flux over incoming momentum flux.|Shapiro}}
Also, Shapiro's Eq 1.15 is identical to Eq 3.42 in the page I linked above. ] (]) 17:05, 4 January 2015 (UTC); edited 17:17, 4 January 2015 (UTC)
I've left "disputed" tags on these two sentences. I am disappointed they were added to the article despite my unanswered question. Please will someone with more specialist knowledge than myself correct them? ] (]) 17:36, 4 January 2015 (UTC)

:My apologies. I took the citation of Shapiro Section 1.5 at its word, as I was not able to check it and you had referred to it as a "minor point". I do think we need to be clear whether each case is allowing a dynamic flow where the net rate of momentum change within the control volume is non-zero, or restricted to a steady-state flow where the net rate of momentum change within the control volume must be zero. &mdash; Cheers, ] (]) 22:17, 4 January 2015 (UTC)

::Thank you, and I'm sorry I didn't make myself clear. By "minor", I meant the content probably needed correcting before release, as opposed to not being inherently useful.

::I think a link to ] may be useful, as I undertsand this momentum theorem directly follows from it.

::In this case, I would be a little uncomfortable with adding material to the encyclopedia which I only learned myself yesterday, in the course of verifying another's work. ] (]) 07:44, 5 January 2015 (UTC)

:::First to ]'s question: Is '''F'''<sub>S</sub> = '''F'''<sub>B</sub> the intended meaning of the last two sentences of the first paragraph of the new section? No. That interpretation isn't consistent with what the variables represent.

:::'''F'''<sub>B</sub> is the body force acting throughout the volume of the fluid, which for an electrically neutral fluid is just gravity. In aerodynamics we usually neglect both gravity and the background hydrostatic pressure gradient that goes with it, under the assumption that they cancel each other. Thus '''F'''<sub>B</sub> = 0 results from neglecting gravity. Whether the flow is steady or unsteady has nothing to do with it.

:::'''F'''<sub>S</sub> is the sum of the surface forces (pressure and viscous shear stress) acting on the control volume boundaries. In the airfoil analyses I've cited it includes both the -L' imposed by the foil and the integrated pressure force on the outer boundary. The volume integral I refer to in the sentences in question is the integral of the material rate of change (]) of momentum in the interior, which is not at all the same thing as '''F'''<sub>B</sub>. Note that the two integrals on the RHS of equation 3.42 of represent the volume- and surface-integral parts of d'''M'''/dt. The fact that d'''M'''/dt has two parts has nothing to do with the decomposition of '''F''' into '''F'''<sub>B</sub> and '''F'''<sub>S</sub>, and the first term on the RHS is not equal to the first term on the LHS.

:::So yes, '''F'''<sub>B</sub> = 0, so that '''F''' = '''F'''<sub>S</sub>, but it's because we neglect gravity, and not because the flow is steady. And no, '''F'''<sub>S</sub> = '''F'''<sub>B</sub> does not follow, and is not the intended meaning of the last two sentences of the first paragraph of the new section. These two sentences follow from the fact that the first integral on the RHS of Shapiro's Eq 1.15 is zero for steady flow, and that the entire RHS represents the same quantity as the RHS of the first equation (unnumbered) of section 1.5, i.e. the instantaneous time rate of change of the momentum of the ''material'' system that occupies the control volume at time t, commonly referred to as the ''material derivative''. The two sentences don't "need correcting". They are consistent with Shapiro, and the "disputed" tags should be removed.

:::The ] as described in the linked article is similar to Shapiro's Eq 1.15, but it uses d/dt to represent a more general kind of time derivative, the total time derivative for some quantity contained within the volume as it evolves in time, including the effects of movement of the boundaries of the volume in the general case. The result is formally the same as Shapiro's only for the special case in which the boundaries of the volume move with the flow as described under "Form for a material element". I think this article is unlikely to help anyone understand Shapiro because it provides less supporting detail than Shapiro does.

:::] wrote:

::::"I do think we need to be clear whether each case is allowing a dynamic flow where the net rate of momentum change within the control volume is non-zero, or restricted to a steady-state flow where the net rate of momentum change within the control volume must be zero."

:::Are you saying that The Statement dp/dt = -L can be true only in unsteady flow? That would make no sense. Actually, all of the sources we list that bear on the dp/dt issue analyze the flow in the frame of the foil and assume the flow is steady in that frame. But the rate of change of momentum within a control volume that's stationary in that frame can still be non-zero in Shapiro's sense of the material derivative. And although Chris Waltham and the AAPT don't say so explicitly, dp/dt in their versions of The Statement has to be referring to the material derivative. Otherwise, if it referred to the conventional partial derivative with respect to time at a fixed location, it would be zero for steady flow, as you say, and The Statement would be false for any control volume. And even I'm saying that there's one control volume for which The Statement is true. ] (]) 06:40, 7 January 2015 (UTC)
::::I am certainly not saying that, as you say that would make no sense. Equations applicable to dynamic momentum distribution will presumably differ from the simpler equations required for steady state. Some of the remarks posted or referenced appeared to encompass the dynamic situation, and that concerned me. For example your new material contains this: "The momentum theorem states that the integrated force exerted at the boundaries of the control volume (a surface integral), is equal to the integrated time rate of change (material derivative) of the momentum of fluid parcels passing through the interior of the control volume (a volume integral). For a steady flow, the volume integral can be replaced by the net surface integral of the flux of momentum through the boundary." Grammatically, the addition of the caveat "For a steady flow" to the second sentence would suggest that the first sentence encompasses unsteady, aka dynamic, flow. Since the momentum theorem is not yet properly defined and cited, I cannot judge whether this is so. Some other materials left me similarly concerned. I have no knowledge of such dynamic situations, nor any references on my bookshelf, or I would be able to comment more sensibly. &mdash; Cheers, ] (]) 12:14, 7 January 2015 (UTC)


::::I see my assumption that each term on the LHS of (3.42) as discussed equates to the same term on the RHS doesn't necessarily follow from what is written, but that's how I read it. Anyway, this equation shows the total force is equal to a volume integral plus a surface integral and it requires some calculation to follow your argument. In shorthand (with the integral contents omitted), Shapiro's Eq 1.15 is ∑F = ∂/∂t ∫<sub>c.v.</sub> + ∮<sub>c.s.</sub>

::::As you say, In steady flow the first RHS term disappears, so<br>∑F = ∮<sub>c.s.</sub>

::::The first equation of 1.5 <ins>is a statement of Newton II in the x-direction. In general Newton II is</ins> <br>∑F = d/dt (mV)

::::So<br>d/dt (mV) = ∮<sub>c.s.</sub>

::::I'm starting to think this wording may not be incorrect, so I have changed the tags. <ins>However, Shapiro 1.5 doesn't directly state any of the three equations above. </ins>

::::The wording in question is:
::::{{quotation|The momentum theorem states that the integrated force exerted at the boundaries of the control volume (a surface integral), is equal to the integrated time rate of change (material derivative) of the momentum of fluid parcels passing through the interior of the control volume (a volume integral). For a steady flow, the volume integral can be replaced by the net surface integral of the flux of momentum through the boundary.}}

::::<ins>The idea that either of the relationships derived above for steady flow conditions are "The momentum theorem" is not consistent with any of the sources I have seen.</ins>

::::I don't see where Shapiro says that d/dt (mV) is the "material derivative" or that this term involves a volume integral.

::::Your assertion that in the discussed (3.42), "the first term on the RHS is not equal to the first term on the LHS" implies that neither term on the RHS is equal to the corresponding term on the LHS. Yet the quotation above seems to imply the opposite: i.e. the second term on the RHS (a surface integral) ''is'' equal to the surface forces, "the integrated force exerted at the boundaries of the control volume" and "the net surface integral of the flux of momentum through the boundary".

::::Anyway, this discussion has already taken up far more of my time than I wish. I am not going to embark on an undergraduate course in Fluid Mechanics just so I can continue to protect this article from dubious and misleading information, as I have done for many months now. ] (]) 12:09, 7 January 2015 (UTC); last edited 06:54, 9 January 2015 (UTC)

::::Also, says, {{quotation|Physically, the linear momentum equation states that the sum of all forces applied on the control volume is equal to the sum of the rate of change of momentum inside the control volume and the net flux of momentum through the control surface.}}
::::] (]) 15:46, 7 January 2015 (UTC)

::::From a reader's perspective, all he needs to know in this context is that in steady flow, momentum changes to air passing through the control volume can be accounted for at its boundaries. I think a simpler form of words would be more understandable. ] (]) 07:43, 8 January 2015 (UTC)
:::::Looking at other sources, as far as I can tell the momentum theorem states that the integrated rate of change of momentum within the control volume equals the sum of the integrated forces acting on the internal volume plus the integrated forces acting on the surface. (e.g. George Emanuel; Analytical Fluid Dynamics, Second Edition, pp447-448 ) That is rather different from the definition currently given in the article. One can add that for a steady state flow where the force acting on the interior is zero, the integrated rate of change of momentum within the control volume equals the integrated forces acting on the surface, like this:
:::::{{quotation|The momentum theorem states that the integrated rate of change of momentum within the control volume equals the sum of the integrated forces acting on the internal volume plus the integrated forces acting on the surface. For a steady state flow where the force acting on the interior is zero, the integrated rate of change of momentum within the control volume simply equals the integrated forces acting at the boundary.}}
:::::I would be happy for this to replace the "wording in question" quoted above. Any objections? &mdash; Cheers, ] (]) 16:35, 9 January 2015 (UTC) ] (]) 16:59, 9 January 2015 (UTC)]

::::::Thanks for suggesting a new wording and for the further reference. All the sources I've seen have presented the momentum theorem in the same form . I see this equates a force to the sum of volume integral and surface integral components of momentum, but I'm not sure how to express it accurately in words. ] (]) 07:01, 10 January 2015 (UTC); edited 07:06, 10 January 2015 (UTC)
::::::If the suggested wording can be reliably cited, I've no objection to its addition to the article. ] (]) 11:55, 10 January 2015 (UTC)
:::::::Specific wording does not need to be cited verbatim (or we would fall foul of plagiarism), however their meaning needs to be clear and that meaning needs to be cited properly. This is what I have tried to do. &mdash; Cheers, ] (]) 12:35, 10 January 2015 (UTC)
::::::::Without plagiarising, we must somehow present the facts which are directly supported by the sources. Does Emanuel say the Momentum Theorem is:
::::::::* the splitting of momentum into surface and volume components of force (14.1)
::::::::* the splitting of momentum into surface and volume components of momentum (14.2)
::::::::* the splitting a force into surface and volume components of momentum (14.3)
::::::::* something else derived later?
::::::::I'm pretty certain some of those bullets are not the correct answer, but I'm not sure which is. ] (]) 13:11, 10 January 2015 (UTC)
:::::::::Emanuel gives the equation of integrals. I paraphrased that equation in words. The LHS is the momentum-change integral, the RHS is the sum of the two force integrals, effectively your 14.1. One could write the equation, which is not plagiarism but equally is not especially helpful unless one explains it in words as well. It would be better included in an article on fluid dynamics in general. &mdash; Cheers, ] (]) 13:31, 10 January 2015 (UTC)
::::::::::I was attempting to describe Emanuel's 14.1, not make my own. I agree the suggested text above is also a verbal description of that equation. My question is whether that equation is in fact "The Momentum Theorem", since Emanuel describes it as "Newton's second law". ] (]) 14:49, 10 January 2015 (UTC); edited 15:39, 10 January 2015 (UTC)
:::::::::::Ah, silly me. My apologies. I'll have to find time to digest Emanuel a bit more carefully. We also have 14.9 to consider. &mdash; Cheers, ] (]) 16:56, 10 January 2015 (UTC)

::::::::::::A lot of issues to deal with here. To begin: ] wrote:

:::::::::::::"I don't see where Shapiro says that d/dt (mV) is the "material derivative" or that this term involves a volume integral."

::::::::::::Good point. He doesn't explicitly use the term "material derivative", though that is the widely accepted term for the kind of time derivative he refers to as d/dt(mV). He also doesn't explicitly say the term involves a volume integral, but he does define it as "the time rate of change of the total x-momentum of the system", which for non-uniform flow can be quantified only in terms of a volume integral. Shapiro's notation is confusing in this regard, and Emanuel would be a better source to cite. The RHS of his eq 14.2 is the same quantity as Shapiro's d/dt(mV). It is clearly a material derivative (for which the capitalized D/Dt is the common notation), and it is clearly a volume integral. So I think my wording is correct and well supported by Emanuel, just not well supported by Shapiro. Thanks for pointing this out.

::::::::::::] wrote:

:::::::::::::"<ins>The idea that either of the relationships derived above for steady flow conditions are "The momentum theorem" is not consistent with any of the sources I have seen.</ins>"

::::::::::::I don't understand your basis for saying this. Your relationship <br>∑F = ∮<sub>c.s.</sub> is identical to Shapiro's eq 1.15, for the case of steady flow, where the first term on the RHS is zero. And this is the final equation in a section headed "Working Form of Momentum Theorem".

::::::::::::] wrote:

:::::::::::::"Your assertion that in the discussed (3.42), "the first term on the RHS is not equal to the first term on the LHS" implies that neither term on the RHS is equal to the corresponding term on the LHS. Yet the quotation above seems to imply the opposite: i.e. the second term on the RHS (a surface integral) ''is'' equal to the surface forces. "

::::::::::::You're right about what is implied, but that doesn't mean it's contradictory. The two second terms are equal only in the special case in which the flow is steady, for which the first term on the RHS is zero, and the body force (the first term on the LHS) is neglected, as it usually is in aerodynamics. This is the special case used in all of the airfoil analyses.

::::::::::::] wrote:

:::::::::::::"From a reader's perspective, all he needs to know in this context is that in steady flow, momentum changes to air passing through the control volume can be accounted for at its boundaries. I think a simpler form of words would be more understandable."

::::::::::::This is also a good point. I originally included the wording about the volume integral of the material derivative because that's the form of the momentum theorem that relates to the "time rate of change of momentum of the air" in The Statement in the intro section, and I think I had the editing community in mind more than the general reader. I agree that the simpler form is better for the article, and I've made the change in my sandbox ].

::::::::::::] proposed replacing "the wording in question" with the following:

:::::::::::::"The momentum theorem states that the integrated rate of change of momentum within the control volume equals the sum of the integrated forces acting on the internal volume plus the integrated forces acting on the surface. For a steady state flow where the force acting on the interior is zero, the integrated rate of change of momentum within the control volume simply equals the integrated forces acting at the boundary."

::::::::::::There are two reasons this isn't satisfactory:

::::::::::::1) As I explained before, setting the body-force term ("the sum of the integrated forces acting on the internal volume") to zero comes from neglecting gravity and has nothing to do with whether the flow is steady or unsteady.

::::::::::::2) This version doesn't mention the surface-integral form for the momentum term, which is the form used in the airfoil analyses that follow.

::::::::::::] asks which of the equations is actually the "momentum theorem". I think a reasonable reading of the sources is that the "momentum theorem" can be expressed in several forms and that it can be any of the equations that relate the integrated force to the integrated rate of change of momentum and/or momentum flux. In Emanuel that would be eq 14.1, 14.3, 14.4, or 14.9. It is ''not'' eq 14.2, 14.5, 14.6, 14.7, or 14.8 because they deal with forces or momentum changes separately, not with the second-law relationship between them.

::::::::::::In light of the above discussion I have changed the words in question to the simpler form suggested by ], and cited both Shapiro and Emanuel. See in my sandbox ]. ] (]) 00:19, 11 January 2015 (UTC)

===The Statement and Newtonian theories of lift===
Regarding the proposed deletion of The Statement, I see nothing in Misplaced Pages policy that says that something "must" remain in an article just because it's already there and has a citable source. Nor do I see anything that says that removal of something that has a citable source requires a direct and citable refutation. No, it looks to me like we as editors are free to make changes based on weighing the sources available to us, even if those sources don't explicitly refer to each other. So it appears to me that ]'s contention that The Statement "must stay" is unfounded. If I'm wrong, show me the specific policy wording.

When ] insists that "mainstream sources" support The Statement, he's being unduly selective. Yes, ''some'' of the sources support The Statement in unapologetic form, but all of the sources taken together, on balance and weighted according to the quality of their analyses, clearly show that The Statement is true only with qualifications. If we present The Statement without the qualifications, we're presenting a biased and misleading impression of what sources on this topic actually say.

The only published analyses we have that support The Statement in unapologetic form are based on the "firehose" model for the flow (Chris Waltham and Clancy). In my posts of 17and 19 December I presented detailed arguments as to why these sources should be accorded less weight than those that use the classical model based on uniform flow plus a vortex. I invited specific counterarguments and so far there have been none.

Likewise, ] invited ] and ] to elaborate on what they think "the air deflected downward" means. Only ] responded, and his answer amounted to "It means whatever it has to mean to make The Statement true, depending on what flow model you prefer". That's an unsatisfactory answer in general, but especially when one of the models we're considering (the "firehose") assigns an unrealistic spatial distribution to dp/dt, as Clancy himself admits.

This is not a question of a choice between a "momentum model" and a "pressure model", as a matter of style or personal taste. No, a proper application of the momentum theorem requires that all of the forces exerted on the air be taken into account, including the pressure force. The "firehose" analyses ignore the pressure force, while the classical analyses properly include it. Thus in terms of the basic physics, these two types of analysis are not of equivalent quality. ] suggests that the new section on Newtonian models "needs a balancing critique of the other simple model we introduce, viz. the pressure model." No, there is no "balancing" of that kind to be done. The classical model is not just a "pressure model". It accounts for both momentum and pressure, and assigns them their realistic locations in the field. It has no faults that rise to the same level as the faults of the "firehose" model. If you disagree with this assessment, please state your specific counterarguments.

The classical analyses (Durand, Batchelor, and Lissaman) clearly deserve more ] than the "firehose" analyses. And they clearly show that The Statement in unapologetic form is misleading. Thus it should either be deleted or properly qualified. This is not "a view unsubstantiated by reliable sources". It is a conclusion supported by an appropriately weighted and balanced consideration of all of the sources. Nor does it constitute synthesis, though I would also argue that the (]) policy doesn't apply to a decision to omit something.

I agree with shortening the heading to "Integrated momentum balance in lifting flows". Regarding the overall organization of "Mathematical theories of lift", I think it's best just as it is, starting with the basic principles, followed by the predictive theories (the ones that actually predict lift starting with the airfoil shape). Those that merely relate one thing to another but don't make actual predictions, such as the Kutta-Joukowski theorem, the momentum-balance analyses, and the Newtonian theories, are not theories at the same level as the predictive theories and should not precede them. This is an ordering that befits an encyclopedia article as opposed to a textbook.

The "Newtonian theories of lift" belongs where I proposed putting it, at the end of Mathematical theories....". None of it should be moved to the introductory section.

] (]) 06:40, 7 January 2015 (UTC)

:Doubters of ] may find it useful to read ] and, on the matter of neutrality, ]. &mdash; Cheers, ] (]) 12:14, 7 January 2015 (UTC)

:Re-reading the proposed section on Newtonian theories of lift, it is really two unconnected parts. The first is a summary of early theories and would go better as the start of a "Historical development" of theories of lift, the second is a critique of the firehose model and while that might be a useful topic to work in somewhere, frankly I find the treatment presented to be unbalanced. Neither part is fit to be moved into the present article as it stands, nor do I intend to engage with the author on their improvement. &mdash; Cheers, ] (]) 12:47, 7 January 2015 (UTC)

::Your feedback that you don't see the connection between the two parts of "Newtonian theories...." is useful. Thank you. I have revised the second part to make the connection clearer. See ]. Beyond that, I have already explained why I struck the balance I did in my criticism of the firehose model. If you have specific suggestions for improving the balance, let's hear them. Simply calling the treatment "unbalanced" isn't helpful.


By way of analogy, regarding flipping a coin we could write:
::You are the only one who has expressed opposition to including "Newtonian theories...." in the article, so at this point yours would seem to be a minority view. Does anyone else oppose my adding this new subsection? ] (]) 00:26, 11 January 2015 (UTC)


:This is because the assumption of it always landing heads-up is wrong. There is no physical principle that requires a coin to always land heads-up and experimental results show that this assumption is false.
== Proposed re-draft of "Flow deflection and Newton's laws" ==


I don't think that anyone would read that as claiming that coins ''never'' land heads-up, only that they don't ''always'' land heads-up. Likewise, ETT is not a general physical principle, but that doesn't imply that it never happens. I don't think we need this level of clarification and the recently added/changed language seems to me to make the section more difficult to read. Perhaps we could simply add a sentence to the effect of "ETT does occur in some situations, but when it does there is no lift." But I don't know that it's really necessary. I'll wait for other editors to weigh in before reverting the edit. ] (]) 14:24, 12 June 2024 (UTC)
Doug McLean recently proposed a re-draft of this section, however it was not met with much support. (personally, I'd support it were there consensus to go in that direction) I've created another draft that will hopefully move us in the direction towards consensus:
https://en.wikipedia.org/User:Mr_swordfish/Lift#Flow_deflection_and_Newton.27s_laws


:Prior to my recent edit, Misplaced Pages’s emphasis was that equal transit time (ETT) is wrong, false, incorrect, misleading etc. In fact, the opposite is true. ETT represents the flow past most solid bodies. Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT. It is only lifting flows that don’t exhibit ETT. Let’s say 99% of flows around solid objects can be described as exhibiting ETT; and only 1% of flows cannot be described in this way. Saying “the assumption of equal transit time is wrong” is a statement that can be soundly challenged unless it is clear that it is confined to lifting flows.
The main ideas are:
:ETT is a very simple 3-word expression. Doug McLean describes it as “an argument that is widespread in explanations aimed at the layman.” (See ''Understanding Aerodynamics'', section 7.3.1.4) A more sophisticated way of saying ETT is “the ] is equal to zero”. There are many reliable sources that talk about flows where circulation is equal to zero.
:Prior to my recent edit, Misplaced Pages said {{tq|there is no physical principle that requires equal transit time ...}} This statement can be soundly challenged unless it is clear that it is confined to lifting flows. The ] is a fundamental theorem in the field of aerodynamics and it clearly implies that a non-lifting flow around a body must have a circulation of zero! Similarly it implies that if the circulation is zero, the lift will also be zero. For circulation equal to zero, the layman may read ETT.
:Misplaced Pages needs to say that ETT does not exist around a lifting body or around an airfoil experiencing lift but we need to be careful to avoid versions of this statement that are so universal in their applicability that they can be readily challenged. It can be challenged if Misplaced Pages implies that ETT is inherently false, or universally inapplicable. ETT is the usual state of affairs, and it is only in the very narrow field of lifting flows that it does not prevail and cannot be assumed. ] ''(])'' 06:15, 13 June 2024 (UTC)
::> ''Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT.''
::Is this true? Usually power lines, wires in fences, and flagpoles sway and move in the wind. What force is causing that movement? Do raindrops always fall straight down, or is there sometimes asymmetrical airflow that causes a horizontal force?
::Flows with zero circulation are nice simple models so there are lots of textbook examples of that idealized condition. I'm highly skeptical that they occur in nature as the rule rather than the as a first order model in theory; for it to occur, I think you'd need to have the solid object be perfectly symmetrical, not rotating, and the airflow non-turbulent. Perhaps you can provide a reference for your 99% claim? Regardless, this tangent distracts from the main thrust of the section i.e. ETT is not a physical law like conservation of momentum, energy, or mass so it can't be assumed.
::The previous version states that "the ''assumption'' of ETT is wrong". That's correct. And "There is no physical principle that requires ETT" That is also correct. We should stick by that. ] (]) 12:56, 13 June 2024 (UTC)
:::Interesting article that addresses the history of ETT. It's not peer reviewed so we can't cite it as a reliable source, but worth a read.
:::https://arxiv.org/pdf/2110.00690
:::'''On the Origins and Relevance of the Equal Transit Time Fallacy to Explain Lift'''
:::Graham Wild
:::School of Engineering and Information Technology, UNSW ADFA, Canberra, Australia
:::G.Wild@ADFA.edu.au
:::1st of October 2021
:::Preprint
:::Not Peer Reviewed
:::Abstract
:::Recently, aerodynamics syllabi have changed in high schools, pilot ground training, and even
:::undergraduate physics. In contrast, there has been no change in the basic theory taught to
:::aeronautical or aerospace engineers. What has changed is technology, both experimentally and
:::computationally. The internet and social media have also empowered citizen science such that
:::the deficiencies in the legacy physics education around flight and lift are well known. The long-
:::standing equal transit time (ETT) theory to explain lift has been proven false. If incorrect, why
:::was it ever taught? Through a historical analysis of relevant fluid and aerodynamics literature,
:::this study attempts to explain why ETT theory is part of our collectively lower-level cognitive
:::understanding of lift and flight. It was found that in 1744 D’Alembert himself assumed this to
:::be a feature of moving fluids, and while this initial intuition (ETT 1.0) was incorrect, the
:::property of ETT (ETT 2.0) was derived in 1752 when applying Newton’s laws of motion to
:::fluids. This incorrect result was independently confirmed in 1757 by Euler! The conclusion is
:::that an over simplified treatment of fluids predicts ETT, along with no lift and drag. This then
:::leads to the open question, can ETT be taught at an appropriately low level as an explanation
:::for lift? ] (]) 12:51, 14 June 2024 (UTC)
:::I don’t accept your arguments. I explained my arguments in significant detail but you haven’t engaged with that detail or responded to it adequately. For example, I have written about non-lifting flows and you have responded with a little original research suggesting that flows with zero circulation are non-existent or rare.
:::If you wish, you could make a reasonable defence of the sentence I amended by arguing that the surrounding context makes it clear to all readers that the entire section, and the article, apply exclusively to lifting flows so if Misplaced Pages says {{tq|the assumption of ETT is wrong}} it is not referring to non-lifting flows. I won’t automatically buy that argument but perhaps I will eventually if it is explained persuasively. It is an argument that has much greater potential than the arguments you put forward in your previous edit.
:::You have written “the assumption of ETT is wrong. That’s correct.” No, it’s not correct in the case of non-lifting flows. I have explained that in detail.
:::You have written “There is no physical principle that requires ETT. That is also correct.” No, it isn’t correct. The Kutta&ndash;Joukowski theorem is a physical principle and it requires ETT in non-lifting flows. I have explained that in detail. ] ''(])'' 13:13, 14 June 2024 (UTC)
::::I think we both agree that ETT is not a valid assumption for an airfoil with lift. I think we also both agree that there is a body of scholarship that does make the simplifying assumption of ETT in some specific examples. That doesn't imply to me that ETT is the usual state of affairs any more than the assumption of a ] implies anything about the shape or real-world cows.
::::You assert that "ETT represents the flow past most solid bodies". But you have not provided a citation for that. I'm highly skeptical that this is true since just about everything moves and flutters in the wind. As Norman Smith's paper states:
:::::...the claim that the air must traverse the curved top surface in the same time as it does the flat bottom surface...is fictional. We can quote no physical law that tells us this.
::::That is, ''in general'' there is no physical law that requires ETT. That's not to say it never happens, or that no physical models ever make that simplifying assumption (and when they do, the result is zero lift). Whether "most solid bodies" exhibit ETT is somewhat orthogonal to this section, so perhaps we don't need to settle that here. I do think that the recent additions and changes are a distraction and make the section less readable. I'll take a look at improving the readability while keeping your concerns about overstating the invalidity of ETT. ] (]) 16:04, 14 June 2024 (UTC)


:::::You and I both have a thorough understanding of the ]. I believe the expression “equal transit time” may be a layman’s way of saying the ] is equal to zero; I hope we agree on that.
* I think we all agree that there is ''a'' region of air for which dp/dt = -L. The draft uses ''a'' instead of ''the''; by using the indefinite article I hope to avoid the confusion that may result in referring to "the air" without specifying what is meant by "the air".
:::::A small part of the problem is that ETT is not a well-defined or rigorously defined expression. To the best of my knowledge this expression is only used by authors who are repudiating this attempt at an explanation of aerodynamic lift. To the best of my knowledge none of the authors and institutions that resort to this naïve explanation of lift actually use the expression “equal transit time“; no-one actually asserts that “ETT” is true or correct. There are only people like us who assert that ETT is not correct (when applied to a body generating lift.)
* I've added a cite which I believe is sufficient to support the language that is in the draft:
:::::Your quote from Norman Smith describes a body with “the curved top surface” and “the flat bottom surface.” He is not referring to “most solid bodies” - he is describing an airfoil!
::"...if the air is to produce an upward force on the wing, the wing must produce a downward force on the air. Because under these circumstances air cannot sustain a force, it is deflected, or accelerated, downward. Newton's second law gives us the means for quantifying the lift force: F<sub>lift</sub> = m∆v/∆t = ∆(mv)/∆t. The lift force is equal to the time rate of change of momentum of the air." Norman F. Smith "Bernoulli and Newton in Fluid Mechanics" The Physics Teacher 10, 451 (1972); doi: 10.1119/1.2352317 http://dx.doi.org/10.1119/1.2352317
:::::I can supply a quotation from Anderson’s “Fundamentals of Aerodynamics” that will help on this topic. I expect to get access to my copy of Anderson within 7 days. ] ''(])'' 14:30, 15 June 2024 (UTC)
* I've moved some of the material around so that the first paragraph deals with the third law and the second paragraph deals with the second law. That seems like a logical organization.
::::::Agree that ETT is not well defined, and that it doesn't appear to be used other than by those repudiating it. Searching for the phrase (or even the word "equal") on my user page collection of works presenting ETT as correct only finds that in the references, not the actual works themselves. Similarly, the obstruction explanation is sometimes derisively referred to as "hump theory" but it's proponents don't use that phrase.
* Some other minor tweaks such as referring to the 'air flow above the wing' rather than the 'air that follows the upper surface'
::::::A typical turn of phrase is "The air moving on the top has to travel a greater distance in the same amount of time." or "Air flowing over the top has a greater distance to travel in the same time; that's why it flows faster."
::::::I don't know that the expression “equal transit time” is a layman’s way of saying the ] is equal to zero, since I would surmize that those advancing the idea probably don't know what circulation is. That said, here's a source basically confirming that ETT and Γ=0 are the same idea.<ref>{{Cite book | title = Flight Physics: Essentials of Aeronautical Disciplines and Technology, with Historical Notes | date = 2009 |edition = 1st | publisher = Springer | location = | isbn = 1-4020-8663-6 | pages = 144 | quote = In conclusion, there is no possibility that the particles passing above and below the aerofoil would arrive simultaneously at the tail, except for the case that there is no circulation around the section – in this case, there is no lift on it. }}
::::::</ref>
::::::Regarding whether most flows around solid objects exhibit ETT, if that were true than ] and ] would not pose problems for engineers to overcome.


::::::{{Reflist-talk}}
I invite the other editors to comment. I hope that I have crafted language that is technically correct, explains the momentum transfer idea as recommended by the AAPT, and is understandable by the lay reader. Suggestions for improvement cheerfully accepted. ] (]) 20:44, 7 January 2015 (UTC)
] (]) 16:20, 15 June 2024 (UTC)


:::Edits finished. Hopefully that addresses the concerns above. ] (]) 16:36, 14 June 2024 (UTC)
:I did edit the article section to include some of Doug McLean's minor suggestions and, from that perspective, I am happy with it as it is. I do not think that Mr. Swordfish's version changes the substance in any way. No version can please everybody, so I have no strong opinion as to whether we stick with what we've got or go for Mr. Swordfish. Either way, the new citation is useful. &mdash; Cheers, ] (]) 21:36, 7 January 2015 (UTC)
::::Your recent edit to the article is an acceptable alternative to my edits. Thank you for making those changes.
::::The article now avoids giving readers the impression that ETT is inherently false. Hopefully readers can now see that the only falsehood is suggesting ETT exists in the flow around a ''lifting body''. ] ''(])'' 14:46, 15 June 2024 (UTC)
:Thanks for the reference to “Flight Physics:Essentials ...” I was not aware of that publication. It looks like it might be essential!
:Vortex induced vibrations are an oscillatory phenomenon. They become a problem in structures that have inadequate stiffness or inadequate damping. In our article on lift we are talking about steady flows with zero viscous effects, or only minor viscous effects. We use a reference frame attached to the airfoil or solid body so the consequences of oscillations of a solid body are way beyond the level of analysis we are using in this article, and related articles.
:Could it be that after half a lifetime of believing that ETT is false, the work of the devil, it will take a major change of direction to accept that there is nothing false or distasteful about ETT? Could that be why you are finding reasons to deny the inevitability of flows in which circulation is zero, ETT prevails and lift is zero? ] ''(])'' 03:46, 16 June 2024 (UTC)
::It's not that I don't believe lift can be zero (and that implies ETT). I just don't think it occurs as often as you seem to think it does i.e. 99% of the time a solid body is immersed in a moving fluid. That's because almost all real world objects are not perfectly symmetrical and that implies an asymmetrical air flow hence non-zero circulation.
::Stated another way, ETT is not a valid assumption in general. If you assume ETT, you will get zero lift. I don't have a cite for this and I am willing to consider evidence to the contrary, but real-world airflows around solid objects with zero circulation are the exception rather than the rule. For instance, consider a symmetrical airfoil in a steady flow - it is well established that the lift varies by the angle of attack. For the special case of zero AOA, the lift is zero and ETT occurs (in this simple 2-d model). For all the other values there is lift, circulation is non-zero, and ETT is false. In mathematical terms, the set of values for which ETT holds has ]. That's about as rare as you can get without it being ''never''.
::Perhaps there is some area of aerodynamic research that assumes ETT or decides that lift is small enough that lift is negligible - many treatments ignore viscosity, or compressibility for example - I'm not aware of any that assume zero lift, but maybe there are. Let me know if you know of any. ] (]) 13:00, 16 June 2024 (UTC)
:::There are several elements of your edit on which I can comment but at present I only have time for one. I will comment on others later.
:::You write about “real-world solid objects with zero circulation ...” Then you make a sneaky gear change and write about “a symmetrical airfoil ...” The two are very, very different in aerodynamics so your gear change doesn’t go unnoticed. Yes, a well-designed airfoil will produce lift (and lift coefficient and circulation) that varies approximately linearly with angle of attack. The feature of a well-designed airfoil that yields this desirable property is the sharp trailing edge. Clancy’s book ''Aerodynamics'' addresses the role of the sharp trailing edge and the way it causes vortex shedding to adjust the strength of the bound vortex to maintain the ]. I don’t have Clancy with me but I think it is Section 4.5 and/or 4.8 that contains good explanatory diagrams.
:::In the absence of a sharp trailing edge, any change in orientation of a body is not accompanied by a change in lift (or lift coefficient or circulation.) For example, a cylinder with elliptical cross section, immersed in a flow produces little or no lift; altering the orientation of the cylinder doesn’t produce much change. What lift might be produced is due to asymmetric boundary layers and separated flow, rather than due to the primary flow predicted using an inviscid fluid. If a body doesn’t have a sharp trailing edge, and the orientation of that body is changed, the fluid flow adjusts itself so that circulation remains zero. Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge. Airfoils have sharp trailing edges, but real-world solid objects don’t. That is why the only circulation and lift that are observed on bodies without sharp trailing edges is the small amount caused by asymmetric boundary layers on the two sides of the body, separated flow and possibly other minor viscous effects.
:::Scientists and engineers have to work hard to generate circulation and lift. Typically they use airfoils with thin, sharp trailing edges even though this feature is structurally weak and vulnerable. Flowing fluids are uncooperative - as they flow around bodies their natural state is doing so with zero circulation. Any change in orientation of a real-world solid body causes the fluid to change its flow pattern to avoid circulation developing. If it were not so, aircraft designers would use wings with thick, generously rounded trailing edges so they could get more fuel into the wings, use deeper and lighter spars, and have more room into which to retract the undercarriage. ] ''(])'' 16:18, 16 June 2024 (UTC)


::::On the matter of the sharp trailing edge there is a very useful quotation by George Batchelor in the short article ].
::I appreciate the work ] has done here to try to bring us together. But although this proposal is less bad than the current version, it doesn't fix the problem. True, "a volume of air" isn't as likely to be misinterpreted as referring to the atmosphere as a whole, but it still begs the question: What volume of air does it refer to?


::::There is also a useful quotation by Richard von Mises at ], reference number 4. ] ''(])'' 00:38, 17 June 2024 (UTC)
::Couching The Statement in terms of "a volume of air" instead of "the air" or "the air deflected downward" changes the substance a bit, but not much. And it still gives prominence to the quote from Cliff Swartz, which makes The Statement in its most unapologetic form, a statement that I've said all along and ] has recently argued is problematic.


::::The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation. Picture the wind blowing around such a body, and then the wind changes direction. Imagine that this change causes a circulation to begin in the flow. This circulation causes a lift force to act on the solid body. Newton’s 3rd law tells us that an identical lift force acts on the flowing air. When a fluid that is free to flow or change shape is subjected to a force or pressure it responds in whatever way will cause that force to diminish. Consequently the lift force on the air flowing around the solid body causes the streamlines, velocities and pressures to change to diminish the circulation that has just begun. This process can be expected to continue until all circulation has been eliminated. Only then has equilibrium been achieved within the flow pattern around the body.
::We've been through this over and over, and I thought that recently ] had come to agree with me on this: The only assumption for which authoritative published analyses have shown The Statement dp/dt = -L to be true, i.e. the tall sliver control volume, is so specific that making The Statement without spelling out the assumption is misleading. The proposed new wording doesn't get us past this problem.


::::Any residual circulation and lift is not related to the primary flow as would exist in a geometrically similar situation but with an inviscid fluid. It is related to the secondary flow caused by viscous effects such as flow separation. Any residual lift is still accompanied by the original drag force. The lift to drag ratio is so small that this solid body doesn’t qualify as an airfoil. I believe this is an explanation for the operation of oddly shaped ] which glide without conventional wings. ] ''(])'' 05:22, 17 June 2024 (UTC)
::If we're going to make the quantitative statement dp/dt = -L, we must spell out what body of air it's true for. The wording wouldn't have to be overly technical or mathematical, but it would have to be specific. Here's my idea of the minimum that would be required to replace ]'s second paragraph and to be technically correct:
::::I'm continuing this discussion since I think I may learn something. I'm not trying to be "sneaky", just trying to understand what evidence there is that zero-circulation/zero-lift/ETT is the usual or normal state of affairs rather than a rare exception.
::::''>Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge.''\
::::Agree that Kutta condition requires a sharp trailing edge, because without one it's not obvious where the rear stagnation point occurs. And without that it's not clear how much circulation to apply to model the fluid re-joining at the rear stagnation point. But you don't need a sharp trailing edge to have an asymmetrical airflow with non-zero circulation, you just can't apply the Kutta contidion. As Gale Craig states, (paraphrasing) ''you don't need an airfoil shape to get lift, as anyone who has ever handled a sheet of plywood in the wind knows.'' Of course, if you want enough lift to fly a plane of propel a sailboat, you'll want something with ''more'' lift than a non-arifoil can provide. That doesn't mean only airfoils with sharp trailing edges can generate lift.
::::I have sailed boats with rudders that have a rounded trailing edge. Performance is sub-optimal, but the rudder most definitely provides enough lift to steer the boat. When I look at leaves on trees or flags on a flagpole in the wind, they never settle down into an equilibrium of zero lift as you describe above. Spinning balls have lift, as any tennis player understands. Here in the US, there's a baseball pitch called the knuckleball where the ball is thrown with a little spin as possible, with the effect that it's impossible to predict which direction the lift will take the ball making it very hard to hit. So, my experience is quite at odds with your assertions.
::::You say that "The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation." but don't provide anything to back that up. Along with your 99% figure, I would need some more to go on than your assertion.
::::Agree that my examples above are anecdotal or original research. Here's an interesting treatment of bluff bodies which seems to be in conflict with your assertion that ''Circulation greater than zero requires the Kutta condition...''
:::::For bluff bodies, the interest is usually in the drag on that body, mainly because experiments have found that drag is the dominant force. This observation, however, does not imply that bluff bodies cannot produce lift because many do. Nevertheless, examining just the drag characteristics of such bodies is convenient in the first instance. Furthermore, bluff bodies may also produce pitching moments, which sometimes need to be known for certain types of engineering work, e.g., to determine torsional loads.
::::] (]) 13:56, 17 June 2024 (UTC)
:::::Here's an excerpt from another paper


<blockquote>
:::In accordance with Newton's second law, some of the air surrounding the airfoil is accelerated downward. The rate at which downward momentum is imparted to the air can be calculated, but it depends on what portion of the air is included in the accounting. Depending on the shape of the region considered, pressure differences acting on the outer boundary of the region offset some of the downward force exerted on the air by the airfoil, reducing the rate at which momentum is imparted, as described below under "Momentum balance in lifting flows". For a column of air that extends to large distances above and below the airfoil and is relatively narrow, the pressure differences are not a factor, and the rate at which downward momentum is imparted is equal to the lift.
:::::Bluff bodies are obviously also subjected to forces in the across-wind direction and to


:::::moments around the various axes due to non-symmetries of the pressure distribution on their
::This gets the momentum-transfer message across in a more accurate way, and it isn't that much longer than the current version or the proposed draft. It cites a different set of sources (Lissaman, Durand, Batchelor) from the proposed draft (Swartz, Clancy, Smith), but I've already made detailed arguments as to why that reflects an appropriate weighting. I would still prefer to keep this section qualitative, an option that both ] and ] have said they could live with. But if we are to make a quantitative Statement, I'd urge you to consider a version with a technically correct qualification, as suggested above.
:::::surface. Therefore, these loads depend fundamentally both of the body shape and on the
:::::orientation of the incoming freestream. Particularly in the two-dimensional case, the force
:::::component in the across-wind direction is often called lift force, in analogy to the
:::::corresponding force acting on an aeronautical wing section (airfoil).
:::::(elision of details about the starting vortex and consequential circulation around an arifoil)
:::::Coming back to bluff bodies, the above described mechanism does not apply in all its
:::::details, particularly because the boundary layer cannot remain attached to their surface even
:::::after the end of the initial transient. However, if the body is sufficiently elongated (like an
:::::ellipse), a starting vortex is shed anyway (even if not as strong as that of an airfoil), and the
:::::asymmetry of the final flow configuration for non-symmetrical wind orientations may be
:::::sufficient for producing significant lateral forces.


</blockquote>
::] (]) 01:14, 11 January 2015 (UTC)
:::::Seems to me that if it were the case that almost all bluff bodies experience zero lift the paper would say that at some point. ] (]) 14:32, 17 June 2024 (UTC)
:::::One of the frustrating aspects of discussing this subject is the variation in meaning given to the word “airfoil”. On these Talk pages I see the word used with three different meanings:
:::::#A two-dimensional shape that can be employed in three-dimensional bodies to generate lift. For example, the shape known as NACA 2412 is an airfoil section commonly used for the wings of low-speed aircraft.
:::::#A three-dimensional body that generates at least a little lift. Some Users point to an irregular body or a sheet of plywood or a sycamore seed and, noting that it experiences a small lift force, say “see, it is an airfoil!”
:::::#A three-dimensional body that, over a usable range of angle of attack, is capable of generating significantly more lift than drag. With this meaning, airfoils are manmade structures that have the generation of lift as their primary purpose. Airfoils are carefully designed and manufactured structures to ensure the lift-to-drag ratio is high enough to achieve its intended purpose.
:::::Misplaced Pages’s current definition of airfoil closely matches No 3 above. ] says:
:::::{{tq|When the wind is obstructed by an object such as a flat plate, a building, or the deck of a bridge, the object will experience drag and also an aerodynamic force perpendicular to the wind. This does not mean the object qualifies as an airfoil. Airfoils are highly-efficient lifting shapes, able to generate more lift than similarly sized flat plates of the same area, and able to generate lift with significantly less drag. Airfoils are used in the design of aircraft, propellers, rotor blades, wind turbines and other applications of aeronautical engineering}}
:::::The layman imagines that the essential feature of an airfoil (meaning No 3) is its generously rounded leading edge, or its curved surface. In fact it is the trailing edge. That is partly the explanation of why a flat sheet of plywood will experience lift in a flow of air - it has a sharp trailing edge.
:::::Since the days of Joukowski and Kutta, mathematicians and physicists have been able to model the flow of an inviscid fluid around suitable geometric shapes. With a sharp trailing edge it is possible to determine the lift and pitching moment on the shapes. Tests on real models of wings in wind tunnels show there is close agreement between the math and the real world for these shapes with sharp trailing edges. For bodies without a sharp trailing edge, the math shows that an inviscid fluid imparts no lift or pitching moment to the body.
:::::Wind tunnel tests on bodies without sharp trailing edges, and anecdotal evidence, show that these bodies can experience a little lift. This does not mean they qualify as airfoils under meaning No 3 above. Engineering, and most science, have little interest in these bodies. What lift they develop is not due to ''airfoil action'' - exploiting the Kutta condition to generate lift. It is due solely to viscous effects such as flow separation. These bodies, at best, have a very low lift-to-drag ratio. Little is written about them in mainstream science or engineering publications. This type of lift has little or no engineering application.
:::::We know that eating a tablespoon of salt a day won’t cure cancer, but it is probably impossible to find a reliable published source that confirms eating a tablespoon of salt a day won’t cure cancer! Similarly it is probably impossible to find a reliable published source that confirms that no bluff body has ever been found that is capable of a high lift-to-drag ratio.
:::::We use the Kutta condition to determine, mathematically, the circulation around a 2-D shape with a sharp trailing edge edge. There is no similar model, theory or equation to determine circulation around a 2-D shape with no sharp trailing edge. I suspect that wind tunnel tests would not show a usable relationship because, being reliant entirely on viscous effects, the results would be strongly influenced by the surface conditions of each model being used - roughness, smoothness, manufacturing imperfections etc.
:::::When I say that bodies without sharp trailing edges do not generate circulation in fluid flows around them, I am speaking as an aerodynamicist applying the model of the inviscid fluid. There is no doubt that my statement is true for inviscid flows, which admittedly are fictitious, but this is usually a good, simple guide to the reality of high Reynolds number flows. When you say that all bodies in a fluid flow experience viscous forces and these forces will provide at least a very small amount of circulation that cannot be eliminated by the flow pattern adjusting itself you are possibly speaking as a scientist focussed on observing the complex realities of the real world. You aren’t able to determine how much circulation there will be, or say exactly how that circulation is sustained. What circulation exists is small and I say it is zero. You possibly describe the same situation by saying circulation is not zero. That might be as close to consensus as we can hope to reach. ] ''(])'' 15:39, 17 June 2024 (UTC)
::::::Agree that I am sometimes a bit loose with the terminology re: airfoil. One other possible avenue of miscommunication here is that when I see the word "lift" in this context I think of the definition used in the first sentence of the article:
:::::::When a ] flows around an object, the fluid exerts a ] on the object. '''Lift''' is the ] of this force that is perpendicular to the oncoming flow direction.
::::::and as a mathematician rather than an aerodynamic engineer ''lift=0'' means actually zero, as opposed to "too small to be useful or significant." One of the arts of engineering is to figure out what things can be ignored, and for most non-airfoil applications the fact that there is some component of the aerodynamic force perpendicular to the airflow is negligible. I'm sure that there are many situations where we would agree that whatever small amount of lift might be present, it's too small to matter so let's assume it is zero. This would imply ETT in that situation.
::::::Other situations I wouldn't agree that it's too small to matter, for instance, a leaf on a tree in a breeze - the leaf repeatedly flutters back and forth in a direction perpendicular to the airflow and this implies to me that there is some force making it move that way and the obvious one is that there is some non-zero component of force transverse to the airflow. I would call that "lift" according to the definition above. But since I doubt either of us will be hired as an engineer to design tree leaves any time soon we can leave it there. ] (]) 17:56, 17 June 2024 (UTC)
:::::::Thanks. I agree with most, if not all, of what you have written. I now realise that the concepts of streamlines, time slices, circulation and ETT are all concepts that rely on steady flow. When we are talking about a turbulent wake, separated flow, oscillatory flow, the erratic dancing of the leaves and branches of a tree, we can’t claim the protection offered by retreating to steady flow. Debating about streamlines, time slices and ETT in a non-steady flow is deeply flawed.
:::::::The dancing of leaves on a tree is definitely caused by the interaction of aerodynamic forces and elastic forces within the highly flexible structures of a tree. This kind of motion could be caused entirely by drag, so I’m not persuaded that the dancing motion of a leaf necessarily shows the presence of lift.
:::::::The concepts of lift and drag rely on knowing the direction of the local velocity of the fluid. The air moving through the branches and leaves of a tree is highly disorganised and the velocity at each point is changing rapidly so it is probably true to say that while we can possibly identify aerodynamic forces acting on branches and leaves, the concepts of a drag component and a lift component are not applicable. The distinction between a lift component and a drag component seems to be reliant on steady flow, and flow in which the speed and direction at one point is almost identical to the speed and direction at all nearby points.
:::::::The Kutta-Joukowski theorem is remarkably similar to Newton’s 1st and 2nd laws. Scientists and engineers say Newton’s laws are valid. Perhaps a mathematician and philosopher might say Newton’s 1st law is redundant because there is no such thing as a body whose acceleration is truly zero; and no such thing as a body experiencing a net force that is truly zero. ] ''(])'' 00:30, 18 June 2024 (UTC)
::::::::In my edit dated 15 June 2024 (14:30) I wrote “I can supply a quotation from Anderson’s ''Fundamentals of Aerodynamics'' that will help on this topic.” See the . In section 3.16 Anderson writes about the Kutta-Joukowski theorem: <blockquote>"Although the result given by the equation <math>L^\prime = \rho_\infty V_\infty\Gamma</math> was derived for a circular cylinder, it applies in general to cylindrical bodies of arbitrary cross section."</blockquote>
::::::::
::::::::This confirms that the Kutta-Joukowski theorem is not confined to airfoils. It applies to all cylindrical bodies regardless of their cross sectional shape. If a cylinder of arbitrary cross section causes no circulation in the flow in which it is immersed the cylinder will experience no lift.
::::::::
::::::::It is not too great a leap to say that, just as airfoils are associated with the Kutta condition to explain when they will generate lift, and when they won’t, cylindrical bodies of arbitrary cross section also rely on a feature resembling a sharp edge to obtain a well-defined lift. If these bodies of arbitrary cross section experience lift in the absence of a sharp edge, it is due to viscous effects such as flow separation and asymmetric boundary layers, rather than due to airfoil action.
::::::::My mention of a well-defined lift is from "sharp trailing edge to obtain a well-defined lift" as written by ]. See citation No. 4 in ]. ] ''(])'' 12:44, 30 June 2024 (UTC)

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Lift force: New Theory of Flight

The following information to the reader is being removed by Dolphin51

1. There is no commonly accepted explanation of the generation of large lift at small drag of a wing as expressed as late as 2020 in Scientific American as “No one knows what keeps planes in the air”.

2. Any reference to the peer reviewed published work New Theory of Flight, Journal of Mathematical Fluid Mechanics, 2017, by Hoffman and Johnson, which offers a new explanation, is being removed.

What is the motivation to hiding 1 and 2 from the public? SecretofFlight (talk) 07:00, 31 July 2021 (UTC)

1. The Scientific American article titled “No-one can explain why planes stay in the air” is an article that has been seen here before, and has been analysed in some detail. We weren’t much impressed. See Humility in the face of the unknown.
If you want to initiate a discussion about this Scientific American article you are welcome to do so on this Talk page, but you can see how it has been regarded in the past. Dolphin (t) 07:44, 31 July 2021 (UTC)
2. I reverted the following text: A New Theory of Flight first presented in Computational Turbulent Incompressible Flow as a new explanation of the generation of large lift at small drag of a wing based on computing turbulent solutions of Euler's equations supported by mathematical analysis, has been developed by J. Hoffman, J. Jansson and C. Johnson. See my diff.
This text said almost nothing about the new theory of flight, but it gave prominence to the authors. On Misplaced Pages, the authors of cited sources are not identified in the article, but they should be identified in an in-line citation.
If you are one of Hoffman, Jansson or Johnson, or you have a close association with them, there may be a Conflict of Interest.
There may be a case for adding this information to the article but it should be added in accordance with encyclopaedic standards. I recommend you have a look at some or all of the following:
Regards, Dolphin (t) 08:57, 31 July 2021 (UTC)

The book Understanding Aerodynamics by Doug McLean gives hard evidence that a common agreement on a scientific explanation of the generation of large lift at small drag of an airplane wing is missing, as just one piece of evidence to this very remarkable fact expressed in the Scientific American article. Why should Misplaced Pages hide this state affairs from the public?

Why is any reference to the New Theory of Flight, which gives the first full scientific explanation backed by solid math and computation, , removed?

Are you open to a section explaining the essence of the New Theory of Flight? Yes I am one of the authors (Johnson). — Preceding unsigned comment added by SecretofFlight (talkcontribs) 08:59, 31 July 2021 (UTC)

You have written about a "common agreement on a scientific explanation of ... lift ..." You have also referred to "this very remarkable fact". In the past decades we have seen many examples of people who believe there can only be one truly correct explanation of aerodynamic lift. These people seem to think "my explanation is correct so all other attempts at explanation must be incorrect." Similarly, there is no reason to expect that scientists will reach agreement on one truly correct way to explain aerodynamic lift. The majority of Users who work regularly on the topic of lift reject as nonsense these suggestions that there is only one truly correct explanation of lift. We also reject as nonsense the suggestion that scientists should reach agreement on one explanation of lift, or that there is something mysterious or sinister in the fact that different scientists display expertise in different ways to explain lift.
The reason your edits have been erased has nothing to do with wishing to hide your theory from public view - it has everything to do with the way it is written and presented in the article. To see how a theory should be written and presented, look closely at the various theories already firmly entrenched in the article - see Sections 2, 4 and 6 in the list of Contents. Also look at the 5 guidance articles I linked in my previous edit. Of course we are open to a section covering a new theory of flight - but it needs to be written in a way that is compatible with the encyclopaedic standards applied across Misplaced Pages. I recommend you draft the section and present it on this Talk page, or on your own personal sandbox, and then use the Talk page to invite interested Users to peruse it and make their comments.
Please remember to sign your Talk page edits with four tildes. Dolphin (t) 13:06, 31 July 2021 (UTC)
Your latest addition to the article (see the diff) looks like an advertisement for a book or a public lecture, rather than a scholarly entry in an encyclopaedia. It contains no in-line citation of the kind required on Misplaced Pages. You have written "The new theory reveals the true physics of generation of large lift ..." The true physics - wow, that is a bold claim indeed! It is not an appropriate claim to make on an encyclopaedia, especially when you have correctly revealed that you have a potential conflict of interest in all matters of the New Theory of Lift.
I suggest you look carefully at the existing content of this article and revise your additions so they look consistent with the rest of the content. Dolphin (t) 13:19, 31 July 2021 (UTC)
It also only cites one primary source and a self-published source. According to the manual of style's guidance for reliable sources:
Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.
So, the latest edit fails to meet basic inclusion criteria. Mr. Swordfish (talk) 23:06, 31 July 2021 (UTC)

I appreciate that I can have a discussion with Misplaced Pages on the important scientific question about "what keeps planes on the air" citing Scientific American 2020 reporting that "nobody knows". The fact that this question does not have a proper answer more than 100 years after the take off of powered human flight in 1903 is very remarkable, impossible to understand for the general general public, and kept as a secret kept within the scientific community of fluid dynamics hidden from the public. Yet it is true, and the evidence is massive. There is no convincing theory of flight in the standard scientific literature, and this is clearly evidenced by the Misplaced Pages article on Lift presenting lots of material but no theory claimed to be correct, because there is none. If there was a correct theory, known to be correct, then Misplaced Pages would present this theory and all incorrect theories now being presented would serve no role. The New Theory of Flight is a new scientific theory for the generation of lift at small drag of a wing with massive support from computation and mathematical evidence developed by leading academicians and published in leading peer reviewed journals opening a new window in the AIAA HiLift Workshops. Misplaced Pages can here serve an important role to expose this new theory to the scientific community for scrutiny and the general public for information. Can we agree on this mission?SecretofFlight (talk) 18:39, 31 July 2021 (UTC)

Regarding the Scientific American article, it's a pretty clear case of journalistic malpractice. John D. Anderson said "There is no simple one-liner answer to this...” The author misrepresented his statement as "What Anderson said, however, is that there is actually no agreement on what generates the aerodynamic force known as lift." which is a completely different statement.

This was further compounded by the headline writer (often headlines are written by someone other than the author of the article, so I don't know precisely who to blame here) who turned that into the sensationalist click-bait headline "No One Can Explain Why Planes Stay in the Air" It's utter crap. That said, if the author had turned down the hyperbole there's a decent article there.

Regarding Hoffman et. al. to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. As such it's WP:FRINGE. Perhaps that will change, but until it does, their work doesn't belong in the article. Maybe Doug can add some perspective here.

While it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic, from internal combustion engines to cheese making. There's nothing mysterious going on here - there are very well established models of lift that are quite well understood, at least by practicing aerodynamic professionals. What has happened is that for the better part of the 20th century the most common simple explanation turned out to be just plain wrong, and when that was pointed out, people being human held tightly on to it because nobody ever wants to admit that they were wrong. Much debate and argument followed, with disagreement on how best to take a complex subject and explain it simply. That's very different than "nobody knows" or even "there is no agreement on the (mathematical) theory." Were we to propagate the "nobody knows" shibbolleth we'd be remiss in our duties as wikipedia editors. Mr. Swordfish (talk) 21:46, 31 July 2021 (UTC)

Yes, it is a good idea to call in Doug McLean who has written an excellent book on flight theory with an attempt to come up with something better than the standard theories all know to be incorrect. I have written a post on my blog which I ask you to read and answer the questions posed at the end. Will you do that?SecretofFlight (talk) 11:00, 1 August 2021 (UTC)

Yes, I have read your blog as you requested. I deplore the fact that you have named @Mr swordfish: in your blog in the way you have done, presumably without their consent or prior knowledge. This is immature behavior that is unlikely to find any support in the scientific community.
At the end of your blog you ask several questions. All your questions are rhetorical. I'm sure you don't know what a rhetorical question is, so I will explain. A rhetorical question is one that is asked without any genuine expectation of an answer; usually because no answer exists or because no answer is wanted. For example, "Why do we have to endure this horrible Covid pandemic?" is a rhetorical question. In a genuine scientific or philosophical dialogue people say what they mean; they don't ask rhetorical questions.
I am building a picture of User:SecretofFlight as a somewhat immature and petulant person; someone more interested in advertising his theory than promoting the best quality article on Misplaced Pages. Please grow up or I will stop communicating with you. Dolphin (t) 12:51, 1 August 2021 (UTC)

You say regarding Hoffman et. al to the best of my knowledge this "theory" has not gained broader acceptance in the aerodynamic community. You are not well informed. The New Theory is now through Jansson an important discussion point at the HiLift Workshops collecting world leading competence.

You say that while it true that there is no simple, correct, and complete theory of lift, you can say the same thing about any other minimally complex topic. This is a misconception about what science is. The main objective of science is to give correct explanations of natural phenomena and it is crucial to distinguish correct theory from false theory. The fact that there is no theory of flight accepted as a correct theory is truly remarkable and efforts to cover up this fact is not science and not in the interest of the public. SecretofFlight (talk) 11:20, 1 August 2021 (UTC)

I did not get any answer on my question posed on my blog so I repeat it here: Why does Misplaced Pages censor any reference to the well documented New Theory of Flight in a Misplaced Pages article on Lift (force), which is only an account of old theories all known to be incorrect? I guess the reason is that the Wikipedians exercising the censorship (Dolphin51 and Mr swordfish) do not themselves carry the scientific expertise required to properly evaluate the merits of the New Theory of Flight and so take the simple way out to dismiss it without any scrutiny. But if so, this is not in the interest of the public. If there is a correct theory of flight, it should not be hidden to the people, in particular not to all people relying on safe air transportation. So I add the following question: Which experts are Misplaced Pages relying on, when dismissing/censoring the New Theory of Flight? SecretofFlight (talk) 18:58, 1 August 2021 (UTC)

The very simple answer as to why the material was removed is that it does not conform to the various wikipedia policies regarding notability, sourcing, and possibly conflict of interest. Dolphin and I have provided links to the help pages that clearly explain the policies and the reasoning behind them. I would suggest you read them, especially WP:ORIGINAL, WP:NPOV, WP:VERIFY, and WP:AGF I'd also suggest you drop the allegations of censorship - they just make your case look weak.
I'm sorry that your theory has apparently not attracted the attention you feel it deserves, but wikipedia is not the place to drum up notoriety. In fact it works exactly the opposite way - first the material must become notable, and only then does it warrant inclusion here. In other words, you need to do your PR work elsewhere first; come back when you have the requisite citations. I'll repeat myself, in case you missed it above:
From reliable sources:
Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.
One very clear problem with your edits is that you haven't established notability. Feel free to come back when you can. Mr. Swordfish (talk) 21:30, 1 August 2021 (UTC)

The only reasonable thing to do is to subject New Theory of Flight to scrutiny by some expert such as Doug McLean. My case is strong because I have hard evidence published in leading journals, while the Misplaced Pages article on Lift (force) is very weak as made very clear in the Talk statement above by Doug. The Misplaced Pages article starts out with (see also blog post):

"There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift".

This is very serious disinformation Mr Swordfish. Very serious. You apparently agree with the statement above by Anderson: "There is actually no agreement on what generates the aerodynamic force known as lift". You thus know very well that there is no scientific explanation of lift agreed to be correct (only incorrect ones agreed to be incorrect), yet you let Misplaced Pages inform the people of the World that there is one, or even better that there are many although most (all?) of them are incorrect. You must understand that this against the most basic of all Misplaced Pages principles your refer to: Misplaced Pages should not mislead the people. Who is telling you to do that? To cover up what is a fact reported by experts in serious media.

I want to bring this case to highest level at Misplaced Pages. It is very serious and of great concern to the people. How do I proceed?SecretofFlight (talk) 06:54, 2 August 2021 (UTC)

User:SecretofFlight: To bring this case to the highest level of knowledge of physics at Misplaced Pages you should take it to the Physics Project team (see Misplaced Pages:WikiProject Physics). You can do this by posting your case at Misplaced Pages talk:WikiProject Physics. Dolphin (t) 12:31, 2 August 2021 (UTC)
Another course of action, which will more likely bring it to the attention of the "highest level", is to raise the issue on one of the various noticeboards. There is a process for resolving disputes that cannot be resolved on the talk page, and I think this one qualifies. See https://en.wikipedia.org/Wikipedia:Noticeboards#List_of_Wikipedia's_noticeboards Mr. Swordfish (talk) 13:47, 2 August 2021 (UTC)

Thanks for this information. I will now prepare material to take the case New Theory of Flight vs Misplaced Pages Lift (force) to the Physics Project Team and also to Noticeboards.SecretofFlight (talk) 16:02, 2 August 2021 (UTC)

Please post a link here when you have filed your case(s). Thanks. Mr. Swordfish (talk) 19:11, 2 August 2021 (UTC)
@SecretofFlight: When a dispute exists a User will sometimes post their case in two different places on Misplaced Pages. When this is realised one of the posts gets deleted promptly so Misplaced Pages’s effort is not divided into two places, potentially producing an ambiguous outcome. I suggest you post first on the Project Physics Talk page and see what happens. If you don’t see a suitable outcome after, say a week, then take it to a Dispute Resolution site. If you post at the Dispute site first it is highly likely that you will be asked to raise the matter first with the subject specialists at Project Physics so they have the opportunity to contribute their views, and their views will be highly valued by others who are trying to arbitrate on any dispute. Dolphin (t) 22:26, 2 August 2021 (UTC)
Seems to me that @SecretofFlight: has larger issues with how wikipedia makes these kinds of editorial decisions than what is within the normal set of issues that Misplaced Pages:WikiProject Physics deals with. I'm not sure which noticeboard is the best venue to adjudicate this dispute, but my sense is that he will receive a more thorough response at the noticeboards than at Misplaced Pages:WikiProject Physics. But I'll leave it up to him to choose the venue. Mr. Swordfish (talk) 02:14, 3 August 2021 (UTC)

@Mr. swordfish,Dolphin51: Before I take the case further I pose the following basic questions connecting to e.g the Scientific American article with headline "No One Can Explain Why Planes Stay in the Air. Do recent explanations solve the mysteries of aerodynamic lift?" (i) Is this a correct description of the state of the science of lift according to Misplaced Pages? If not, what is incorrect? (ii) Is there an accepted scientific theory/explanation of the generation of lift at small drag of an airplane wing? If yes, which is this theory/explanation? (iii) Mr. Swordfish states above "It is true that there is no simple, correct, and complete theory of lift". Does this mean that there is a non-simple, correct and complete theory, if so which, or no such thing? (iv) The Misplaced Pages article starts out: "There are several ways to explain how an airfoil generates lift. Some are more complicated or more physically rigorous than others; some have been shown to be incorrect. For example, there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift". There seems to be a contradiction between (i)+(ii)+(iii) and (iv), that is a contradiction between the statements (a) There is a commonly accepted scientific explanation of lift, and (b) There is no commonly accepted scientific explanation of lift. Which of (a) and (b) is the view of Misplaced Pages? I want a clear answer, not handwaving that (c) they are both correct since there are many theories carrying different elements, some true some false. It is against this background the New Theory of Flight stands out as the first explanation in both mathematical and physical terms of the generation of lift at small drag of a wing with solid documentation in the scientific literature, which you remove from visibility on Misplaced Pages. The matter is serious. The role of Wikepedia is to give correct information to the people, not double messages that there both is and is not a scientific explanation of lift. Ok?SecretofFlight (talk) 06:57, 3 August 2021 (UTC)

My views on this matter, and my answers to your questions, are all evident in the posts I have made to this thread. I suggest you take your case further. I will respond there. Dolphin (t) 12:40, 3 August 2021 (UTC)
I agree. We've both already responded to most of this upthread. I fail to see the utility in discussing it further here. Mr. Swordfish (talk) 13:43, 3 August 2021 (UTC)

@Mr. swordfish,Dolphin51: No, you have not answered my questions in your posts! To take the case further it is necessary to make the present standpoint of Misplaced Pages clear on the matter of scientific explanation of lift. You say you will respond in the next instance. I ask you to do this right away, so that we will not have to start all over again. You have a responsibility to all the readers of Misplaced Pages and to the scientific community you are representing to answer my questions. What are your answers? SecretofFlight (talk) 13:59, 3 August 2021 (UTC)

@Mr. swordfish,Dolphin51: If you are unable/unwilling to answer the most basic question concerning the article Lift (force) for which you have responsibility, a question of utter scientific importance, then you are not, as I can see, filling the role of a true Wikipedian, which I think will not be appreciated by Misplaced Pages when made clear in the next instance. Do you see my point? You say that answers are to be found in your posts on this thread. Then point me to them! The world expects clear answers. What are your answers?SecretofFlight (talk) 14:34, 3 August 2021 (UTC)

@Mr. swordfish,Dolphin51: You can choose between two roles as Wikipedians: (i) You can go to history by opening to a much needed scientific discussion on theory of flight with in particular new input from New Theory of Flight, in a situation where there is no commonly accepted correct scientific theory of flight and all current theories basically dating back more than 100 years, are known to both experts and people through popular science press, to be incorrect/incomplete. (ii) You can act as gate keepers with a cover up that for sure there are (many) theories of flight, that science is settled and that New Theory of Flight has no place on Misplaced Pages. Which role do you prefer? For help to come to a decision I invite you to Secret of Flight with in particular the videos The Secret of Flight and Incorrect Theories of Flight. SecretofFlight (talk) 15:26, 3 August 2021 (UTC)

Here is state of art of standard fluid mechanics as expressed by Doug McLean in his book Understanding Aerodynamics concerning scientific understanding of lift:

"So in one sense, the physics of lift is perfectly understood: Lift happens because the flow obeys the NS equations with a no-slip condition on solid surfaces. On the other hand, physical explanations of lift, without math, pose a more difficult problem. Practically everyone, the nontechnical person included, has heard at least one nonmathematical explanation of how an airfoil produces lift when air flows past it. Such explanations fall into several general categories, with many variations. Unfortunately, most of them are either incomplete or wrong in one way or another. And some give up at one point or another and resort to math. This situation is a consequence of the general difficulty of explaining things physically in fluid mechanics, a problem we’ve touched on several times in the preceding chapters."

We read that generation of lift of a wing is a secret deeply hidden in the Navier-Stokes equations with no slip (but uncomputable because of very thin boundary layer), while scientific understanding in physical terms is a difficult problem, apparently unresolved (as expressed in Proposed revision of simplified explanations of lift below).

The New Theory of Flight reveals the secret of lift hidden in the Euler/Navier-Stokes equations with slip (without boundary layer and thus computable) in a description of slightly viscous incompressible flow around a long wing as potential flow modified by 3d rotational slip separation at the trailing edge into a turbulent wake, with potential flow generating large lift by attaching to the upper surface while gliding with very small friction as expressed by slip combined with 3d rotational slip separation at the trailing edge without the pressure rise of full potential flow destroying lift.

In short: Standard CFD as Navier-Stokes with no-slip is uncomputable and hides the secret of lift, while Euler/Navier-Stokes with slip is computable and opens to reveal the true secret in a New Theory of Flight in the form of potential flow modified by 3d rotational slip separation. It is as simple as that. Details on Secret of FlightSecretofFlight (talk) 07:48, 2 August 2021 (UTC).

@SecretofFlight: @Mr swordfish: @Dolphin51: I read "The Secret of Flight" paper and found the description to be compelling but somewhat hyperbolic in its claims. Although this material is not yet covered in secondary sources, it is not fringe, and it is recent and I think sufficiently strong to be included here in the article on lift. I've included a short description towards the end of the article, in Three Dimensional Flow, where it seems to fit best. Please consider keeping it, making changes, or delete it if you think this is not a valuable addition to the article, as I believe it is. Dilaton (talk) 21:52, 15 August 2021 (UTC)

@Dilaton: Thanks for your thoughts on this one. I concede that this new theory might be regarded as sound in some quarters, and might one day be widely accepted among mathematicians as a theory of flight. At present I see nothing to suggest that it is sufficiently mature to warrant mention in Misplaced Pages or any other encyclopaedia aimed at a general audience. We have seen two attempts at describing what this new theory of flight looks like, but I am none the wiser. For example, expressions like:
  • 3D vortices. There appears to be nothing on Misplaced Pages to explain 3D vortices so this expression cannot be linked to any existing article to enable the reader to find something about these vortices. (Is this just an alternative to line vortex or vortex filament? Or is it somehow different?)
  • potential flow modified by 3D rotational slip separation at the trailing edge into a turbulent wake. This is inaccessible to a general audience. It looks like something from a PhD thesis. Misplaced Pages is not the place for such a thesis.
  • the potential flow generates large lift by attaching to the upper surface while allowing a wing to glide with very small drag from turbulent vortex attachment at the trailing edge. Potential flow attached to the upper surface? Surely every application of potential flow around an airfoil since the time of d’Alembert has assumed the flow is attached to the upper surface, and to the lower surface as well? Sentences like this serve more to confuse than to explain.
If it is to earn a place in this article, it must be described in a way that a general audience might comprehend. Despite your best efforts, your recent addition to the article is unlikely to be comprehended by a specialist audience of fluid-dynamic-literate users, much less by a general audience.
My view is that your recent addition should be removed. I will wait to see what Mr swordfish and other Users think. Dolphin (t) 07:35, 16 August 2021 (UTC)
@Dolphin51: Thanks for considering an addition. "3D vortices" is an attempt to convey that these are a collection of vortex filaments of unequal alternating vorticity, with ends attached to the trailing edge. It is essentially a more accurate refinement of the Kutta condition, in which the sheet of shear leaving the trailing edge is now understood as a sheet of turbulent vortices. The improvement of understanding comes in now seeing that this is where the majority of the drag originates on an airfoil. Perhaps the paragraph I attempted to add could be improved with this or other language? Dilaton (talk) 15:38, 16 August 2021 (UTC)
Misplaced Pages policy is abundantly clear that there must be secondary sources to include material. So far, there has been none for the "new theory of flight" despite a decades long PR campaign that often spills over into Misplaced Pages. The academic article itself has been accessed about 720 times and has garnered a total of 6 citations in the literature. Now, it may be that as Dolphin says it "...might one day be widely accepted among mathematicians as a theory of flight." but for now it's not. I've removed it since it clearly does not meet the standards for reliably sourced material. Mr. Swordfish (talk) 14:48, 16 August 2021 (UTC)
@Mr swordfish: I understand your concern and respect your adherence to secondary sources; however, WP:NOR does state that primary sources published in reliable places can be used with care, and I think this published article may thus qualify and be used carefully. Or we can do as you wish and wait for someone else to write about it. I do think that would be a bit of a loss, as the improvement of understanding of drag from attached vortices seems significant. Dilaton (talk) 15:38, 16 August 2021 (UTC)
@Dilaton:While you are correct that primary sources may be used with care, there must be some secondary sources to support notability. At the risk or repeating what I posted upthread, Misplaced Pages policy on reliable sources says:
Misplaced Pages articles should be based on reliable, published secondary sources and, to a lesser extent, on tertiary sources and primary sources. Secondary or tertiary sources are needed to establish the topic's notability and to avoid novel interpretations of primary sources. All analyses and interpretive or synthetic claims about primary sources must be referenced to a secondary or tertiary source, and must not be an original analysis of the primary-source material by Misplaced Pages editors.
Here, we have a paper that was published five years ago and in response the world has shrugged. Now, perhaps it is truly the major scientific breakthrough that the authors claim it to be. Perhaps even you agree that it is and think that the world needs to be told about it. Fine. Go do that. But do it somewhere else. Come back when there are sufficient secondary sources to support the notion that it merits inclusion here. Mr. Swordfish (talk) 23:39, 16 August 2021 (UTC)

I have to say that the sheer volume of debate on these talk pages leads me to believe that the Scientific American article was right after all. --Westwind273 (talk) 05:43, 1 September 2021 (UTC)

The Scientific American article comprises two distinct elements: firstly there is the title “No-one can explain why planes stay in the air.” and secondly there is the body of the article.
My impression of the body of the article is that it contains little to support the title. If you believe the body of the article contains some text addressing what the title says, please let us know what you see - please return to this Talk page and quote the wording you are looking at. Many thanks. Dolphin (t) 05:59, 1 September 2021 (UTC)

Proposed revision of simplified explanations of lift

There is a proposal for a revised treatment of simplified explanations of lift available at

https://en.wikipedia.org/User:J_Doug_McLean/sandbox

I think in general it is very good. I think it could be improved by addressing the following issues:

  1. The current article states "The downward turning of the flow is not produced solely by the lower surface of the airfoil, and the air flow above the airfoil accounts for much of the downward-turning action." This has been removed in the draft. I think it needs to be stated somewhere in the article, otherwise readers may come away with "skipping stone theory"; I'm not seeing a better place than its current location, but I could be persuaded otherwise.
  2. it doesn't adequately present the streamtube pinching explanation. Probably most of us reading this are already familiar with this "explanation" which can be found in Anderson and Clancy, but the typical reader will probably have no idea what we're talking about. The current article does present it, and I think if we're going to include this material we should explain it more fully than the draft does.
  3. it asserts :

    the "streamtube pinching" explanation also starts by arguing that the flow over the upper surface is faster than the flow over the lower surface

    That's not my understanding of the argument. In the current version of the article (which I believe accurately reflects the reliable sources) the streamtube pinching explanation starts with the fact that theory predicts and experiments confirm that the streamtubes narrow on the top of the wing, and proceeds from there.
  4. it lumps streamtube pinching into an "incorrect" subheading, but I'm unconvinced that streamtube pinching is actually incorrect. My view, which I think is born out by the reliable sources, is that it is a correct description of the physical phenomena, but with the logical problem that it begs the question of why the streamtubes change size.
  5. it claims that speed/Bernoulli explanations come in two basic versions, but there is a third: the half-venturi tube "explanation". There are probably others. I think this can be easily written around, assuming we don't want to drag half-venturi into the article, by replacing "These explanations come in two basic versions" with "There are two common versions of this explanation"
  6. The final subsection "Alternative explanations, misconceptions, and controversies" is reduced to only one explanation, misconception, or controversy after moving previously contained material upwards. It might be appropriate to address half-venturi, skipping stone, "squeeze the soap" and others here. Or just remove this subsection.

There are probably some other minor edits to avoid repetition and improve readability, but I think if the issues above are addressed the revised material will be ready for publication. Thanks for your efforts on this. Mr. Swordfish (talk) 00:42, 1 August 2021 (UTC)

Thanks for the feedback. To respond to the issues raised above:
1. Yes, let's put this back. And let's find a source to cite for it.
2-3. I think the whole paragraph taken together describes the arguments correctly, but I see how it can be confusing if you look at the first sentence by itself. I'll try a rewrite. I don't support retaining the current article's opening statement on what experiments and analyses show. It's a true statement, but no reliable source I know of uses it in the context of a streamtube-pinching explanation of lift, and the current article cites no source for it. My objective is still to stick with the classical sources that propose a reason for the pinching, even if we end up pointing out that the reason doesn't make sense.
4. I agree with your comment on "versions". But I still think streamtube pinching belongs under the "incorrect" heading because its two main steps (streamtube pinching causes higher flow speed, and higher flow speed causes lower pressure) run opposite to actual physical cause-and-effect. In addition to not providing a good reason for the pinching, it has the flaw that conservation of mass isn't a satisfying physical reason why the flow would speed up. Really explaining why something speeds up requires identifying the force that makes it accelerate. I'll add the second "flaw".
5. The upper-surface-as-an-obstacle and the upper-surface-as-a-half-Venturi are really the same argument. Your rewording is OK with me.
6. I'm going to try removing the "Alternative explanations..." subhead and move the "Controversy regarding Coanda effect" sub-subhead up with the flow-deflection explanation, as that's the explanation to which it relates.

I've implemented these changes in my sandbox. Thank you for the suggestions. J Doug McLean (talk) 17:23, 4 August 2021 (UTC)

I have gone through the proposed text and I find it excellent, and an improvement over the current state of the article. I have a few minor language/typographic fixes in mind, which I think will be better carried out once the text is integrated in the article. -- Ariadacapo (talk) 07:09, 5 August 2021 (UTC)
Thanks for your consideration of my suggestions.
1. I have added a citation for the assertion that the upper surface produces "much" of the lift. I'd like to find a better one, but I think this will do for now.
2. My working hypothesis is that the vast majority of our readers will not be familiar with the streamtube pinching explanation. It can be found in Anderson's Introduction to Flight, Eighth Edition, but not in earlier editions (or at least I couldn't find it there), in Clancy's Aerodynamics, and in Eastlake's article for The Physics Teacher. I have been unable to find it elsewhere. A year or so ago I was of the opinion that it was sufficiently obscure that it didn't merit attention in the article, but after acquiring Clancy and seeing it there, my opinion has changed. My best guess is that most people who have taken a college level class in aeronautical engineering have seen it, but it remains mostly unknown to the general population.
Since we can't expect the reader to already be familiar with it, we should provide a more detailed description - the current draft states "When streamtubes become narrower, conservation of mass requires that flow speed must increase." This is certainly true, but a sentence or two along with a picture will help many readers to understant why narrow streamtubes imply faster flow.
3. I think you are correct that the current article's treatment is at variance with the sources. Re-reading Anderson, he starts with "obstruction theory" to explain streamtube pinching, not "Starting with the flow pattern observed in both theory and experiments..." so we should present it his way. Eastlake doesn't explicitly explain why the streamtubes change size, but he alludes to the flow passing "the thickest part of the airfoil" and putting your thumb over the end of a hose, so I'll place him in the "obstruction theory" camp. I don't have my copy of Clancy with me and won't for several weeks, so someone else will need to check that reference.
4. The authors of the current section must have been engaging in an act of charity to re-factor the streamtube pinching explanation so that it is not actually incorrect. Seems that we both agree that the current version is not actually incorrect, but it is different than what is to be found in the cited sources. Since the sources present the explanation as a result of obstruction, we should too. And when we do, I think it is appropriate to lump it under the "Incorrect" heading.
One thing I'd like to see carried over from the current article is
Sometimes a geometrical argument is offered to demonstrate why the streamtubes change size: it is asserted that the top "obstructs" or "constricts" the air more than the bottom, hence narrower streamtubes. For conventional wings that are flat on the bottom and curved on top this makes some intuitive sense. But it does not explain how flat plates, symmetric airfoils, sailboat sails, or conventional airfoils flying upside down can generate lift, and attempts to calculate lift based on the amount of constriction do not predict experimental results.
The material expressed in the first sentence has been carried over, but the rest has not. Since the third sentence above is one of the better (best?) arguments why obstruction theory is lacking I think it makes sense to continue to include it.
5. Seems to have been taken care of. Thanks.
6. Moving the Coanda material up and removing the depleted section on "Alternative theories" makes logical sense. My issue with this version of the draft is that the article now spends more time discussing what is essentially a semantic issue than it does treating the much more central idea of lift as a consequence of conservation of momentum. Moving the Coanda material down in the article would be an acceptable solution, but I'm not sure where to move it. Like the streamtube pinching explanation, I think the "Coanda controversy" is limited to folks who have done some formal study or aerodynamics and not widespread in the general population, so perhaps we don't really need to address it. Or perhaps find a more concise way to present it.
Thanks for considering my suggestions. I think we're making real progress here. Mr. Swordfish (talk) 14:28, 5 August 2021 (UTC)
@Mr Swordfish: If at 3. you are alluding to the citation of Clancy p.76 “This lift force ... ... downward momentum of the air” I can confirm that this is an accurate quotation from Section 5.15 Lift and Downwash (which is on p.76 in my copy.) Dolphin (t) 00:19, 6 August 2021 (UTC)
@Dolphin: My recollection is that Clancy presents the streamtube pinching explanation, but I don't recall whether he starts with "obstruction theory" or proceeds from some other premise (e.g. the "theory & experiment" approach the article uses). We don't cite Clancy in this subsection, so you'll have to look beyond our citations. If you have your copy handy, I'd appreciate if you could take a look at Clancy's approach and report back. Thanks. Mr. Swordfish (talk) 18:18, 6 August 2021 (UTC)
@Mr Swordfish: I have had a quick look through Clancy. He explains lift using the Circulation Theory and the Kutta-Joukowsky theorem. The book appears to contain no linking of lift on an airfoil and stream tube pinching. There are several diagrams that show streamlines of varying spacing around a circular cylinder with circulation, and around an airfoil-shaped cylinder with different amounts of circulation. In the explanatory text adjacent to the diagram of the circular cylinder with circulation Clancy draws attention to the varying spacing of streamlines and links this to pressure variation using Bernoulli (Section 4.5 Circular Cylinder with Circulation on p.38) In the text adjacent to diagrams of airfoils Clancy makes no attempt to draw attention to streamline spacing and its implication for pressure.
In para 4.5(b) Clancy writes “The effect of the circulation is generally to increase the speed over the upper surface of the cylinder and to reduce the speed over the lower surface. This effect is shown by the spacing of the streamlines in Fig 4.4”
In para 4.5(c) he writes “From Bernoulli’s Theorem, therefore, it follows that the pressure is generally reduced on the upper surface and increased on the lower surface. As a result, there is a net force vertically upwards. This is lift.” Dolphin (t) 13:49, 7 August 2021 (UTC)
I stand corrected about streamtube pinching appearing as an explanation of lift in Clancy. I'm now back to wondering if presenting this explanation here is giving it undue weight. Mr. Swordfish (talk) 14:17, 7 August 2021 (UTC)

I've been re-reading the Help article on undue weight, first in the context of the streamtube pinching "explanation", but then in the context of the apparent controversy over the Scientific American article that claims "nobody understands lift". The article on weight states

Neutrality requires that mainspace articles and pages fairly represent all significant viewpoints that have been published by reliable sources, in proportion to the prominence of each viewpoint in the published, reliable sources. Giving due weight and avoiding giving undue weight means articles should not give minority views or aspects as much of or as detailed a description as more widely held views or widely supported aspects.

The current version of the article states succinctly "...there are explanations based directly on Newton's laws of motion and explanations based on Bernoulli's principle. Either can be used to explain lift." The proposed revision does an about face and states "...neither approach, by itself, is a completely satisfactory explanation." (And then there's the SA article, which I'm going to ignore as WP:FRINGE.)

Both of these are valid opinions that are supported by reliable sources. I tend to agree with the latter as my own opinion, but when I put on my editing hat I find it problematical to clearly come down on one side or the other. If we're going to present this controversy, we're supposed to present both sides and "teach the controversy". That said, I don't want to waste our readers' time by rehashing the great Bernoulli v Newton debate that raged back in the late nineties. My preferred solution is to sidestep the issue and avoid sweeping statement about whether both are right, or neither is right, (or whether nobody really knows). The proposed revision clearly explains each approach and its limitations or shortcomings. I think the readers can draw their own conclusions without us having to make sweeping statements like the above examples.

I'll copy the present proposal over to my sandbox and make the proposed changes there so we retain an easy to access "clean" copy of Doug's proposal.

Regarding the streamtube pinching, or "obstruction theory", I'm in agreement that it's essentially the same argument as the "half venturi tube" approach, which seems to be more prevalent in the sources so we should give more prominence to it. I'll take a whack at that, along with an attempt to provide a more concise treatment of the Coanda material. Mr. Swordfish (talk) 13:44, 10 August 2021 (UTC)

My view is that there are multiple explanations of lift, each derived from one or more of the various conservation laws and other laws of physics that are applicable to a solid object immersed in the flow of a fluid. We make use of multiple explanations of lift to serve the needs of the multiple audiences that have an interest in the subject. Even within one audience there are multiple purposes and objectives that cannot be satisfied by just one explanation. For example:
  • An explanation of lift that can be presented to 19-year olds will be unsuitable for 13-year olds. An explanation that is both satisfying and satisfactory for student pilots will be unsuitable for students of physics and engineering.
  • An explanation that helps explain lift in 2-dimensional flow will not be satisfactory if the objective is to help explain lift-induced drag.
I support the sentiment in the present article: “Either can be used to explain lift.” I don’t support the sentiment that "...neither approach, by itself, is a completely satisfactory explanation." It will be unhelpful, unnecessary and unsound to apologise for certain explanations of lift, or to suggest that no satisfactory explanation exists, or that no-one knows what it is. Misplaced Pages is able to demonstrate its maturity and soundness by not engaging in a search for a "completely satisfactory explanation". Nor should Misplaced Pages support a notion that every incomplete explanation must be incorrect.
When we search for the most appropriate explanation of lift for our purposes we are engaging in applied science or applied math or engineering but we aren’t engaging in pure or fundamental science. Bernoulli’s principle and Newton’s laws of motion have universal application and so qualify as fundamental science, but an explanation of lift on an airfoil is simply one of many examples of Bernoulli and Newton in action. There will never be a Committee of eminent scientists whose task is to determine by arbitration the one true explanation of lift.
When we talk about the explanation of lift based on Bernoulli’s principle, it would really be more accurate to say we are using lift as an example of Bernoulli’s principle in action. Similarly, when we talk about the explanation of lift based on Newton’s laws, it would really be more accurate to say we are using lift as an example of Newton’s laws in action. The pure science is always more fundamental than the application of that science to one of a multitude of everyday observations.
I look forward to seeing your latest proposal on your sandbox. Dolphin (t) 12:10, 11 August 2021 (UTC)
Dolphin, Agree that different audiences require different explanations, and it is appropriate for us to present several, starting with the easier to understand and proceeding to the more rigorous. I think we need to be careful about using words like "satisfying" and "satisfactory" because they beg the question of "satisfying to whom?" My hunch is that most people are completely satisfied to know nothing about this topic. Those who bother to read the article may come away satisfied after a section or two, or they may read further until they are "satisfied".
Moving on....
The opinion “Either can be used to explain lift.” is just that - an opinion. So is the opinion "...neither approach, by itself, is a completely satisfactory explanation." If we're going to include either one, we need to present the other, present both as opinion, and provide some context for how widespread each is in the reliable sources. I'd rather not do that, especially early on in the article. Perhaps a later section on the "Bernoulli v Newton Controversy" would be in order, or perhaps a separate article instead. My preference is to just sidestep it as a distraction and present the various approaches, starting from simple and moving to the complex, with some context to address whatever shortcomings or limitations each approach has. And let the material speak for itself without making unnecessary sweeping generalizations.
To that end, I don't think we need the first section "Understanding lift as a physical phenomenon". The article starts with qualitative physical explanations without math and proceeds to the various mathematical models. That is apparent from the table of contents, so I don't think we need to state it explicitly; readers will get it if they bother to read that far. I'm going to remove it from my draft. Comments appreciated.
My view is that no version is 100% complete nor is any version 100% correct. When we do physics, we make abstract models, and in order to make the models tractable we make some simplifying assumptions along the way so the model doesn't exactly describe the actual physical phenomena. That doesn't mean that the models are bad, just that they are always limited, and when criticized for that variance the criticism is often warranted. For instance, 2D potential flow doesn't predict stall, drag, or downwash. But it does a surprisingly good job at predicting lift without making the math impossible. IOW, it's a good but limited model.
Which is to say that every explanation is incomplete to some degree. So, I'm not sure it's "fair" to label the explanation based on flow deflection and Newton's laws that way in the title. I do think it's fair to state that it's incomplete in the body, so I'm removing it from the title but leaving it in the body.
Regarding "Bernoulli-based" explanations, the two we discuss in that section are clearly incorrect. Correct explanations involving Bernoulli (or more properly, explanations that are based on models that have some predictive power) always include many other physical principles to the extent that it's a misnomer to call them "Bernoulli-based". To put a finer point on it, they always include conservation of momentum at some level. Bernoulli's principle is just one piece of the puzzle.
That said, I think a serious shortcoming of this draft as it stands is that readers may come away with the notion that Bernoulli's principle is somehow wrong, or that it is always incorrect to use it when explaining lift. I think we need so say something along the lines of "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." But I'm not sure where to put it or how best to phrase. Suggestions appreciated. Mr. Swordfish (talk) 18:32, 14 August 2021 (UTC)
UPDATE: I've added "Although these two simple explanations are incorrect, there is nothing incorrect about Bernoulli's principle, or it's usage in a more complicated explanation of lift." to the draft. Mr. Swordfish (talk) 18:49, 14 August 2021 (UTC)

I've not gotten much feedback on the draft in my sandbox. I'm not sure if that's because other editors don't like it, or because they think it's fine as is. Assuming the latter, I'll give it a couple of days and if no objections I'll deploy the material in my sandbox. Mr. Swordfish (talk) 22:02, 19 August 2021 (UTC)

I will be happy to give some feedback in the next day or two. Dolphin (t) 22:42, 19 August 2021 (UTC)
Thanks. It's more important that we get it right than that we do it fast. But I want to keep the process moving. Mr. Swordfish (talk) 01:41, 20 August 2021 (UTC)
It looks good to me and I don’t see much to comment on. I have provided my feedback at User talk:Mr swordfish/sandbox. Dolphin (t) 13:31, 20 August 2021 (UTC)

I think the proposed new section "Understanding lift as a physical phenomenon" is important. It clarifies the status of the qualitative explanations relative to the rigorous scientific understanding embodied in the mathematical theories. In so doing, it says a lot more than what a reader could infer from the TOC or what he would be likely to realize even after reading the entire article. I think it makes what follows much easier to understand.

I think we should keep the "Obstruction..." explanation. Anderson is a very prominent author, and this book is a prominent source.

I've put up a new candidate in my sandbox. It avoids the "satisfactory" wording and removes the value judgements from the headings. It also incorporates Swordfish's shortened version of the Coanda section and his separate subheads for "Equal transit time" and "Obstruction...". I added another subhead to separate out the issues common to both explanations that had been swallowed into the "Obstruction..." subsection. I also incorporated his wording on Bernoulli not being incorrect as a principle, with the added qualification that Bernoulli is applicable outside the boundary layer. Comments? J Doug McLean (talk) 19:21, 21 August 2021 (UTC)

I've copied Doug's latest draft over to my sandbox for the purposes of comparison. The diff is here: https://en.wikipedia.org/search/?title=User%3AMr_swordfish%2Fsandbox&type=revision&diff=1040264566&oldid=1039805588 I'll have more to say in a day or so. Mr. Swordfish (talk) 17:29, 23 August 2021 (UTC)

Comments on the latest drafts (24 Aug 2021):

o The first thing I noticed when looking at the diff was that the latest version from Doug is some 10,000 characters shorter. This is mostly refs that didn't make it over. I don't think it will be controversial to restore the refs, although some may be ripe for pruning. I'll restore all of them in my next draft, and if any are deemed to be unnecessary we can remove them on a case-by-case basis.

o Regarding the first section , it reads to me as an opinion rather than a simple statement of fact. The current version of the article also includes the opinion that "Either can be used to explain lift." I prefer the simple factual statement in my previous draft, which I think adequately foreshadows the qualitative vs mathematical dichotomy to come.

There are several ways to explain how an airfoil generates lift. Some are more complicated or more mathematically rigorous than others; some have been shown to be incorrect. Most simplified explanations follow one of two basic approaches, based either on Newton's laws of motion or on Bernoulli's principle.

o I looked into other wikipedia articles that link directly to sub-headings, and only found one that would be affected by the current drafts. I added an anchor tag to that section. We should make sure that it makes it into the final version.

o Agree to keeping the obstruction/constriction/streamtube-pinching explanation. While it's not nearly as widespread as the ETT fallacy, it seems to be common enough for us to reference it here (although I'd be open to an argument that it's not if anyone wants to make it). I think it's worth expending a single sentence on NASA's "Venturi tube" version of it since NASA's site may be the most widely read version.

o I don't think labeling the incorrect explanation as "incorrect" is a value judgement. Seems to be simply a statement of fact, so I'd advocate restoring that in the titles.

o I like the additional subhead to address issues common to both - I wanted to do that myself, but couldn't come up with a good title.

o I'm unconvinced that it's necessary to state that "Bernoulli's principle is applicable to the flow outside the boundary layer." at this point in the article. I think simply stating "Bernoulli's principle can be used correctly as part of a more complicated explanation of lift." is sufficient for the intended audience for this portion of the article. If we're going to address when Bernoull's principle applies and when it doesn't, that should wait until later in the article.

o Regarding "This explanation is correct as far as it goes but is incomplete. " I've come to agree with Dolphin's that "as far as it goes" is a colloquial idiomatic expression, that while common in the US may not be understood the way it's meant to by someone unfamiliar with the expression. If we were writing this for a US audience I'd advocate to keep it, but since we're writing for the broader English-speaking world I think the phrase should be excised. We have two candidates for the material at this point:

This explanation is correct but it is incomplete. It doesn't explain how the airfoil can impart downward turning to a much deeper swath of the flow than it actually touches. Furthermore, it doesn't mention that the lift force is exerted by pressure differences, and doesn't explain how those pressure differences are sustained.

and

Flow deflection combined with Newton’s laws is a helpful way to explain some aspects of lift. It leaves some questions unanswered; it doesn't explain how the airfoil imparts downward turning to the flow, and it doesn't mention that the lift force is exerted by pressure differences. It doesn't explain how those pressure differences are sustained.

I prefer the concise "correct but incomplete" phrasing, but could be persuaded otherwise.

I'll merge the the latest draft from Doug with mine, incorporating the ideas above. Comments as always welcome. Mr. Swordfish (talk) 16:32, 24 August 2021 (UTC)

Oversimplification

The current version of that section still refers to Bernoulli's Principle as "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." This sounds great, but it isnt correct, as it is a (fairly significant) oversimplification of his work. In the context of aviation and aerodynamic lift, it is only accurate along a streamline where no heat is being transferred between the wing and the air. Does the cited work include this gross oversimplification? As importantly, does the gross oversimplification make the concept clearer to the reader? PrimalBlueWolf (talk) 08:26, 23 August 2021 (UTC)

@PrimalBlueWolf: Where you have written “but it isn’t correct ...” do you mean Bernoulli’s principle doesn’t correctly represent the reality; or our article doesn’t correctly reflect the principle described by Bernoulli?
It is well known, and always acknowledged in reliable published sources, that Bernoulli’s principle doesn’t take account of viscous forces within the fluid, nor does it apply to a flow field in which heat is being transferred. Despite these assumptions Bernoulli’s principle is a very powerful tool in analysing the subsonic flows around streamlined bodies. I don’t agree with your characterisation that the Misplaced Pages article represents a “gross oversimplification.” Please explain further. Dolphin (<.,span style="color: blue;">t) 13:57, 23 August 2021 (UTC)

That it doesn't correctly represent the principle as represented in Hydrodynamica. The current version of the article alleges that you can determine velocity and pressure of any other point using Bernoulli's Principle knowing only the velocity and pressure of one point, and the velocity of one other point. That is only valid along a streamline, but the article doesn't acknowledge that. PrimalBlueWolf (talk) 21:25, 23 August 2021 (UTC)

It is often stated that "Bernoulli's principle is only valid along a streamline" but this is a misconception. Within a flow field that exhibits uniform flow as the initial condition, BP applies throughout the flow field. This assumes that the energy is constant, i.e. it assumes no heat loss (as one would find in the example of an airplane wing) or no net work done (as one would find in the example of a sailboat). If one is going to pick nits, BP is not applicable to any real world airfoil due to these energy considerations, however it is commonly used as a approximation or simplification to make mathematical models tractable. Physics is full of these approximations, e.g. assuming sin(x)=x for sufficiently small x. And if we're not going to assume constant energy, BP doesn't apply along a streamline either.
The statement "there is a relationship between the pressure at a point in a fluid and the speed of the fluid at that point, so if one knows the speed at two points within the fluid and the pressure at one point, one can calculate the pressure at the second point, and vice versa." is consistent with how BP is used in practice in mathematical analysis of fluid dynamics. Granted, it's a calculational shortcut that does not precisely model the actual physical world. But it's close enough for engineering work. Note that the section is about "simplified explanations" and is not the proper place for a long technical discussion of exactly when BP applies and when it doesn't. Mr. Swordfish (talk) 03:28, 24 August 2021 (UTC)

@PrimalBlueWolf: As you can see, I have moved your posts and the responses from me and @Mr swordfish: to their own thread under this new heading.

You have written “That is only valid along a streamline, …” That is incorrect in the case of a wing generating lift in the atmosphere. Consider the following:

In Fluid Mechanics by V.L. Streeter (1951 McGraw-Hill), section 3.7 The Bernoulli Equation says:

The constant of integration (called the Bernoulli constant) in general varies from one streamline to another but remains constant along a streamline in steady, frictionless, incompressible flow. These four assumptions are needed and must be kept in mind when applying this equation.

Under special conditions each of the four assumptions underlying Bernoulli's equation may be waived.

1. When all streamlines originate from a reservoir, where the energy content is everywhere the same, the constant of integration does not change from one streamline to another and … may be selected arbitrarily, i.e. not necessarily on the same streamline.

In Aerodynamics by L.J. Clancy (1975 Pitman Publishing) section 3.4 Bernoulli's Theorem for Incompressible Flow says:

Further, at some distance upstream of the aircraft, the flow consists of a uniform stream. It follows that on any given streamline in this region the value of p + 1/2 ρ v is the same as it is on any other streamline.

In Fundamentals of Aerodynamics by John D. Anderson (1984 McGraw-Hill) section 3.2 Bernoulli's Equation says:

For a general, rotational flow, the value of the will change from one streamline to the next. However, if the flow is irrotational, then Bernoulli's equation holds between any two points in the flow, not necessarily just on the same streamline.

In the language of fluid dynamics we say Bernoulli's principle applies equally at all points on all streamlines in a region of irrotational flow. A wing operates in a stationary atmosphere so there are no viscous forces or vorticity in the air outside the boundary layers. The flow around a wing is irrotational everywhere except in the boundary layers.

You have also written “… only accurate along a streamline where no heat is being transferred between the wing and the air.” I assume you are referring to transonic and supersonic flow. The Misplaced Pages article presently only refers to lift in subsonic flight. In low-speed flight there is no significant amount of heat being transferred. Dolphin (t) 04:32, 24 August 2021 (UTC)

I'm glad to take the correction and agree with the reasoning. Thanks for the detailed and well sourced explanation. PrimalBlueWolf (talk) 07:19, 24 August 2021 (UTC)

Proposed new version of simplified explanation continued

The last thread had gotten rather long, so starting a new one.

Latest version now available in my sandbox.https://en.wikipedia.org/User:Mr_swordfish/sandbox

I opted to keep the opening section, at least for now, but as it stands now there is substantial repetition between it and the first paragraph of the next section. Not sure what is the best solution, but I'm out of time for the day. Comments and suggestions appreciated. Mr. Swordfish (talk) 15:33, 26 August 2021 (UTC)

I spent some time today looking at other Misplaced Pages articles on technical, mathematical, or scientific subjects. I came away with two observations:
  1. The articles discuss the topic at hand, rather than discussing the article and how it covers the topic.
  2. None of them have language that implies that the topic is difficult to explain or to understand.
With that in mind, the opening section "Understanding lift as a physical phenomena" would be an outlier in terms of Misplaced Pages style. The more matter-of-fact treatment in the section that follows is in keeping with wider Misplaced Pages standards.
See Aerodynamics, Wing, Quantum Mechanics, Fluid Mechanics, Fluid Dynamics, Chemistry, Category Theory for a few examples.
On that basis I'm going to remove the section from the draft while repurposing some of the language into the new first section. At this point, I think we have a release candidate. Comments? Mr. Swordfish (talk) 15:31, 27 August 2021 (UTC)
I agree. I encourage you to release the latest version. Dolphin (t) 13:35, 28 August 2021 (UTC)
It's been released. Thanks to everyone who contributed. Mr. Swordfish (talk) 21:06, 28 August 2021 (UTC)

Sorry for not weighing in sooner on the latest changes. I've been away for a few days.

I see that the proposed new section has been removed again and that some of the language has been "repurposed" into the following section. It seems to me that these changes have negatively impacted the article's organizational clarity. The first mention of the mathematical theories now comes under the heading "Simplified explanations.....", and with this placement the mathematical theories are now categorized as one of "several ways to explain how an airfoil generates lift". This isn't an accurate reflection of where the mathematical theories fit in the overall picture. The mathematical theories are the basis of the rigorous scientific understanding of lift. They're not "explanations" of lift.

I think the proposed new section reflected the facts of the matter more clearly. Except for the phrase (referring to the simplified explanations) "and most readers will likely already have been exposed to one or more of them", which I propose we delete, everything that remains is a straightforward statement of fact. Even the one bit of "meta" information ("These issues are discussed in connection...") is a factual statement that more detail on the issues just raised is coming later in the article, not a "discussion" of "how the article covers the topic".

I don't think that providing a bit of factual meta information is out of place in a Misplaced Pages article. Nor is it out of place to say that a correct qualitative explanation of lift is difficult, given that it's a statement of fact supported by the checkered history of qualitative explanations and by the sources (my TPT paper, at least).

I've tweaked the proposed new section and removed its heading, which makes it part of the "Overview" section, where I think it fits well. I've also taken a crack at removing the resulting duplication from the intro to "Simplified physical explanations..." in my sandbox. My recommendation is to merge these changes into the article in place of the recently released version. J Doug McLean (talk) 19:27, 2 September 2021 (UTC)

Thanks for your continued effort on this page. I've made an attempt to merge your latest version with the current article. It's in my sandbox. https://en.wikipedia.org/User:Mr_swordfish/sandbox#Overview Comments appreciated. Mr. Swordfish (talk) 20:12, 4 September 2021 (UTC)
Mr Swordfish: I have no objection to the current version in your sandbox being released. Dolphin (t) 12:52, 6 September 2021 (UTC)
Mr Swordfish: Your rendition of the addition to "Background" is more cryptic than my draft, but I'm on board with all of it except the last sentence, which seems to me to be ambiguous. Actually, I think all, not just some, of the simplified explanations we present have the flaw of leaving important things unexplained, even the ones that also have incorrect elements. A possible revision:
There are also many simplified explanations, but all leave significant parts of the phenomenon unexplained, while some also have elements that are simply incorrect.
I think we're almost done and on the verge of completing a significant improvement of the article. J Doug McLean (talk) 00:54, 7 September 2021 (UTC)
I have implemented the suggested change in my sandbox and will deploy that version. However, I failed to start with the latest version from the real article and several changes have been made since I deployed the version from my sandbox so I can't just do a cut and paste or it will override those changes. So, there will be several intermediate versions in my sandbox as I reconcile the two. Mr. Swordfish (talk) 13:46, 8 September 2021 (UTC)

Coandă effect criticism

The following sentence was recently added:

A criticism of the Coandă effect as an explanation for aerodynamic lift is that the Coandă effect itself is not well understood.

With a cite to https://digitalcommons.usu.edu/cgi/viewcontent.cgi?article=1096&context=etd

The relevant part of that paper says:

The Coanda effect has been widely used in the both aeronautics and medical applications , air moving technology, and other fields. Nevertheless, this phenomenon is not completely understood, especially for three-dimensional flow as in the CSM design. The nature of the Coanda effect, with boundary layer separation and entrainment interaction, make for difficulty in solving the flow numerically and analytically.

I'm not seeing where the source criticizes the usage of the Coandă effect to explain lift, so this material appears to be WP:SYNTHESIS. A bigger problem is that saying that "the Coandă effect itself is not well understood" is a very broad statement that would need stronger backing than the carefully worded excerpt from the cited Masters Thesis above. Reading the Coandă effect article I don't see anything supporting the assertion that it is not well understood - were this truly the case I would expect it to be treated in that article.

Of course, that wikipedia article is not dispositive - we're supposed to look at reliable sources, and other wikipedia articles are not reliable sources - but it strikes me that if we're going to publish a broad assertion like that the proper venue for discussing it and presenting the source material would be the talk page for that article, not this one.

I'm removing the material pending the production of better citations. Mr. Swordfish (talk) 20:32, 9 March 2022 (UTC)

I agree with Mr. Swordfish that better citations are necessary. However, as far as I have been able to determine, there are no sources that offer a well thought out explanation for why or how the Coandă effect applies to aerodynamic lift. The popular references quoted in the main article (references 33 and 34) certainly do not offer that explanation. This lack of a source making a detailed argument for applying the Coandă effect to aerodynamic lift is not apparent in the main article. I tried to make this deficit of a source argument, not vey well I must agree, but one that should be made. It is difficult to make this argument since there are no referenceable sources that point out this deficit of a source offering a valid explanation. David Weyburne (talk) 16:51, 10 March 2022 (UTC)
Were I writing this article for myself, I'd include something like:
People often try to explain why the air is deflected on the top of the wing by saying it's because of the Coandă effect, but this doesn't actually explain anything, it just gives it a fancy European name.
But I'm not allowed to just make stuff up on my own and I haven't seen this idea expressed elsewhere so I don't have a source for it. And that means I can't add it to the article. That said, I agree with the sentiment that it's poor pedagogy to explain something via material that the reader doesn't understand either. And I think the article would be improved with a short statement like the one above or something similar to what you added, but unless we can find reliable sources to cite we can't add it. If you find a good source for this I'm all ears. Mr. Swordfish (talk) 23:23, 10 March 2022 (UTC)

Anderson and Eberhardt's "Understanding Flight" (McGraw-Hill, 1st ed. 2001) is the one source I know of that appeals to the Coanda effect in a lift explanation and also tries to explain how Coanda works in physical terms. They attribute the Coanda effect entirely to viscous "shear forces." On p. 23, after explaining no-slip at the surface and the resulting formation of a boundary layer, they say:

"The differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer. This causes the fluid to try to wrap around the object."

This explanation of Coanda is easy to rebut. However, my own book ("Understanding Aerodynamics", Wiley, 2012) is the only citable source I know of that does so explicitly. With reference to using Coanda in lift explanations, I say in sec 7.3.1.7:

"The Coanda effect is erroneously seen as implying that viscosity plays a direct role in the ability of a flow to follow a curved surface. Anderson and Eberhardt assert that viscous forces in the boundary layer tend to make the flow turn toward the surface, specifically, as they put it, that the 'differences in speed in adjacent layers cause shear forces, which cause the flow of the fluid to want to bend in the direction of the slower layer.' Actually, there is no basis in the physics for any direct relationship between shear forces and the tendency of the flow to follow a curved path."

In the paragraphs following the above, I explain in detail my reasons supporting the statement in that last sentence. The gist of it is that the curving of the flow is a result of the interaction between the pressure field and the velocity field, as we explain in the article under "A more comprehensive explanation." It has practically nothing to do with viscous or turbulent shear stresses. As long as the boundary-layer doesn't separate, the curving of the flow to follow the curved surface is an essentially inviscid effect.

Mr. Swordfish has invited us to identify a citable source for his naming-isn't-explaining objection to relying on Coanda. Again, the only one I know of is my own book. In sec 7.3.2 I list things to avoid in an explanation of lift. Item 5 is:

"'Naming' as a substitute for explaining, as, for example, in saying that a jet flow follows a curved surface because of the Coanda effect, where 'Coanda effect' is just a name for the tendency of jet flows to follow curved surfaces."

So we have citable sources for a couple of possible additions to the Coanda subsection that would be of interest to some readers. I'm not enthusiastic about doing it, however, because I think we may already be giving Coanda more prominence than it deserves. On the other hand, I could argue that the article as it stands doesn't present enough of the case against Coanda, and that the additions we're considering here would balance things better and help justify the word "Controversy" in the article's section heading.J Doug McLean (talk) 20:20, 3 April 2022 (UTC)

Thanks very much Doug. Mr swordfish and I will ensure your book is cited as a source where it is appropriate to do so in relation to Coanda effect. Dolphin (t) 23:49, 3 April 2022 (UTC)
Now that we have a cite I've been trying to craft language along these lines, but so far haven't come up with anything that doesn't seem out of place or unencyclopedic. I'll keep trying. Suggestions cheerfully considered. Mr. Swordfish (talk) 23:56, 11 April 2022 (UTC)
Mr swordfish and J Doug McLean I have inserted a paragraph that, hopefully, begins to capture some of Doug's wisdom from above. See my diff. Dolphin (t) 04:41, 27 September 2022 (UTC)
I have also added a sentence on "naming is not explaining". Mr. Swordfish (talk) 18:55, 28 September 2022 (UTC)

A new simplified lift explanation

As if things weren't complicated enough, I have developed a new simplified explanation for aerodynamic lift that I would propose as a add-on to the present version. I am looking for comments and recommendations at this point.

The proposed text is available in my sandbox at https://en.wikipedia.org/User:David_Weyburne/sandbox

The proposed explanation is based on a graphical interpretation of the mathematical equations governing fluid flow. The key to the approach is the graphical plots of the velocity profiles and the pressure gradient profiles taken at a bunch of locations along the airfoil surface. This permits a one-to-one correspondence between the flow governing equations and the plotted profiles. By invoking the momentum conservation equation in this way, the explanation provides the connection between the velocity and pressure fields that is missing in the other simple explanations. David Weyburne (talk) 13:38, 17 September 2022 (UTC)

Where a Misplaced Pages User develops a new explanation for something it is called Original Research. Such an explanation is not published in Misplaced Pages - see WP:NOR.
Your explanation cannot be described as simplified. I find it mystifying. Some of your sentences are statements of the obvious and therefore unnecessary in your description; and others are either incorrect or misleading. If you wish to continue with your work on this subject in order to publish it in an appropriate place, it needs a lot of refinement.
You are relying on four sources but three have been published by yourself. This is usually unwise and I have commented at User talk:David Weyburne/sandbox. Dolphin (t) 23:20, 17 September 2022 (UTC)
Thanks for the feedback. As to original research comment: I do not think any of the explanations presented in the Simplified Explanations section would constitute original research that would be appropriate for a journal article. The explanation may be original but it is not something that can be tested and verified by other research groups. As to the rest of the comment: I am sorry you find it mystifying but I am hoping that is not the case for the majority of readers. You claim there are obvious statements that are unnecessary: I have tried to make the explanation readable for the non-expert and would hope that the expert reader would allow for that. You also claim there are misleading and incorrect statements: It is hard to comment on this claim since you did not bother to outline which statements are false or misleading. David Weyburne (talk) 12:54, 21 September 2022 (UTC)
David Weyburne Thanks David. On 18 September I made some introductory comments about statements I regard as superfluous, and others I regard as misleading. Those comments are on one of your Talk pages - see User talk:David Weyburne/sandbox. Dolphin (t) 23:05, 21 September 2022 (UTC)
Sorry, I initially missed your comments in my sandbox. I appreciate your detailed comments and I have replied to the comments in the Talk section. At this point I will leave the explanation as is and would add that a more detailed explanation is available in the supplied references. David Weyburne (talk) 12:40, 22 September 2022 (UTC)
One further note as to the observation that three of the sources were published by myself and is therefore inappropriate. I would point out that one is a YouTube video, another is an Air Force Technical Report, and the third is an e-book collection of my Air Force Tech Reports. All of them lay out a more detailed version of the condensed simplified explanation provided in my Sandbox. The reason the references are all mine is that I believe that my simplified explanation is original. However, as I stated before, this type of simplified explanation is not something that would be appropriate to be published in a standard journal. It is appropriate for providing a simplified explanation in an encyclopedia-style format. David Weyburne (talk) 12:45, 23 September 2022 (UTC)
As the author of the proposed cited articles you may be subject to Wikipeda's conflict of interest policy. I would suggest familiarizing yourself with that policy. I appreciate the fact that you have disclosed that you are the author of those articles, but that fact remains and is germane and therefore not inappropriate.
That said, the fact that the proposed additional material uses your articles as their source doesn't mean that the material can't be added to the article, or that your articles can't be cited. We've encountered this issue before with a prominent author, who provided some very valuable insights into this topic and helped improve the article. But he made very few edits himself, instead working with the other editors to reach consensus about any proposed revision to the article. I think we are on solid grounds if we follow that model. Mr. Swordfish (talk) 19:38, 23 September 2022 (UTC)
Sorry, been busy. I understand that referencing my own work is problematic. To explain the reason for doing this, I need to give a little background. My simplified explanation for aerodynamic lift is based on showing "graphically" how the conservation of mass, momentum, and energy occurs for a flow around an airfoil. To do this, I start using a simple word-based argument to say that mass diversion results in velocity changes while being diverted around an airfoil. These velocity changes result in a speed up for the flow on the airfoil. How do you graphically show this speed-up? It is possible to use streamline, contour, or vector plots of the velocity but because of the large spatial variations, this approach is not very effective. Hence, most simplified explanations for lift regress to simply stating that "the velocity speeds up". For my simplified explanation I switched to a series of "velocity profile plots" along the airfoil. The profiles show the velocity behavior from a point on the airfoil to a point deep in the free stream above the airfoil. What you see are velocity peaks near the airfoil surface that slowly return to the free stream over distances of ~two chords. These peaks are important in that it gives a visual confirmation of velocity changes and give a one-to-one comparison to the momentum equation du/dy term. The momentum equation says these velocity changes must be conserved which is done, in part, by pressure changes. I then can show a plot of the pressure gradient profiles above and below the wing at the same location as the velocity profiles. The difference in the pressure profile areas, the pressure difference, shows graphically how mass and momentum conservation results in lift.
So what is the problem, why do I only reference my own work? The reason is there is no one doing anything similar using velocity profiles. This velocity profile "peaking" behavior is not discussed or plotted anywhere in the literature that I could find (other than the simple text saying "the velocity speeds up"). Many textbooks show schematics of boundary layer profiles but not ones that show the peaks, the velocity speedup behavior. I observe it my airfoil simulations and in raw mesh data provided by other researchers, but nowhere in the literature. If I had references showing that these velocity and pressure profile peaks exist, I would be less dependent on referencing my own work. For the record, I think for the non-expert, my 15 min. graphics-based YouTube video does a better job of explaining this aerodynamic lift argument than my e-book version.
I would be willing to work with any editor to resolve this issue. David Weyburne (talk) 15:03, 23 March 2023 (UTC)

Recent changes to equal transit time section

The diff is here: https://en.wikipedia.org/search/?title=Lift_%28force%29&diff=1228641725&oldid=1227711027

I don't read the previous version as claiming that equal transit time never happens, only that it cannot be assumed. The "offending" passage is:

This is because the assumption of equal transit time is wrong. There is no physical principle that requires equal transit time and experimental results show that this assumption is false.

By way of analogy, regarding flipping a coin we could write:

This is because the assumption of it always landing heads-up is wrong. There is no physical principle that requires a coin to always land heads-up and experimental results show that this assumption is false.

I don't think that anyone would read that as claiming that coins never land heads-up, only that they don't always land heads-up. Likewise, ETT is not a general physical principle, but that doesn't imply that it never happens. I don't think we need this level of clarification and the recently added/changed language seems to me to make the section more difficult to read. Perhaps we could simply add a sentence to the effect of "ETT does occur in some situations, but when it does there is no lift." But I don't know that it's really necessary. I'll wait for other editors to weigh in before reverting the edit. Mr. Swordfish (talk) 14:24, 12 June 2024 (UTC)

Prior to my recent edit, Misplaced Pages’s emphasis was that equal transit time (ETT) is wrong, false, incorrect, misleading etc. In fact, the opposite is true. ETT represents the flow past most solid bodies. Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT. It is only lifting flows that don’t exhibit ETT. Let’s say 99% of flows around solid objects can be described as exhibiting ETT; and only 1% of flows cannot be described in this way. Saying “the assumption of equal transit time is wrong” is a statement that can be soundly challenged unless it is clear that it is confined to lifting flows.
ETT is a very simple 3-word expression. Doug McLean describes it as “an argument that is widespread in explanations aimed at the layman.” (See Understanding Aerodynamics, section 7.3.1.4) A more sophisticated way of saying ETT is “the circulation is equal to zero”. There are many reliable sources that talk about flows where circulation is equal to zero.
Prior to my recent edit, Misplaced Pages said there is no physical principle that requires equal transit time ... This statement can be soundly challenged unless it is clear that it is confined to lifting flows. The Kutta–Joukowski theorem is a fundamental theorem in the field of aerodynamics and it clearly implies that a non-lifting flow around a body must have a circulation of zero! Similarly it implies that if the circulation is zero, the lift will also be zero. For circulation equal to zero, the layman may read ETT.
Misplaced Pages needs to say that ETT does not exist around a lifting body or around an airfoil experiencing lift but we need to be careful to avoid versions of this statement that are so universal in their applicability that they can be readily challenged. It can be challenged if Misplaced Pages implies that ETT is inherently false, or universally inapplicable. ETT is the usual state of affairs, and it is only in the very narrow field of lifting flows that it does not prevail and cannot be assumed. Dolphin (t) 06:15, 13 June 2024 (UTC)
> Airflow past a power line, past each strand of a wire fence, past every flag pole, satisfies the description of ETT. Every rain drop and hail stone that have ever fallen have experienced the 3-dimensional equivalent of ETT.
Is this true? Usually power lines, wires in fences, and flagpoles sway and move in the wind. What force is causing that movement? Do raindrops always fall straight down, or is there sometimes asymmetrical airflow that causes a horizontal force?
Flows with zero circulation are nice simple models so there are lots of textbook examples of that idealized condition. I'm highly skeptical that they occur in nature as the rule rather than the as a first order model in theory; for it to occur, I think you'd need to have the solid object be perfectly symmetrical, not rotating, and the airflow non-turbulent. Perhaps you can provide a reference for your 99% claim? Regardless, this tangent distracts from the main thrust of the section i.e. ETT is not a physical law like conservation of momentum, energy, or mass so it can't be assumed.
The previous version states that "the assumption of ETT is wrong". That's correct. And "There is no physical principle that requires ETT" That is also correct. We should stick by that. Mr. Swordfish (talk) 12:56, 13 June 2024 (UTC)
Interesting article that addresses the history of ETT. It's not peer reviewed so we can't cite it as a reliable source, but worth a read.
https://arxiv.org/pdf/2110.00690
On the Origins and Relevance of the Equal Transit Time Fallacy to Explain Lift
Graham Wild
School of Engineering and Information Technology, UNSW ADFA, Canberra, Australia
G.Wild@ADFA.edu.au
1st of October 2021
Preprint
Not Peer Reviewed
Abstract
Recently, aerodynamics syllabi have changed in high schools, pilot ground training, and even
undergraduate physics. In contrast, there has been no change in the basic theory taught to
aeronautical or aerospace engineers. What has changed is technology, both experimentally and
computationally. The internet and social media have also empowered citizen science such that
the deficiencies in the legacy physics education around flight and lift are well known. The long-
standing equal transit time (ETT) theory to explain lift has been proven false. If incorrect, why
was it ever taught? Through a historical analysis of relevant fluid and aerodynamics literature,
this study attempts to explain why ETT theory is part of our collectively lower-level cognitive
understanding of lift and flight. It was found that in 1744 D’Alembert himself assumed this to
be a feature of moving fluids, and while this initial intuition (ETT 1.0) was incorrect, the
property of ETT (ETT 2.0) was derived in 1752 when applying Newton’s laws of motion to
fluids. This incorrect result was independently confirmed in 1757 by Euler! The conclusion is
that an over simplified treatment of fluids predicts ETT, along with no lift and drag. This then
leads to the open question, can ETT be taught at an appropriately low level as an explanation
for lift? Mr. Swordfish (talk) 12:51, 14 June 2024 (UTC)
I don’t accept your arguments. I explained my arguments in significant detail but you haven’t engaged with that detail or responded to it adequately. For example, I have written about non-lifting flows and you have responded with a little original research suggesting that flows with zero circulation are non-existent or rare.
If you wish, you could make a reasonable defence of the sentence I amended by arguing that the surrounding context makes it clear to all readers that the entire section, and the article, apply exclusively to lifting flows so if Misplaced Pages says the assumption of ETT is wrong it is not referring to non-lifting flows. I won’t automatically buy that argument but perhaps I will eventually if it is explained persuasively. It is an argument that has much greater potential than the arguments you put forward in your previous edit.
You have written “the assumption of ETT is wrong. That’s correct.” No, it’s not correct in the case of non-lifting flows. I have explained that in detail.
You have written “There is no physical principle that requires ETT. That is also correct.” No, it isn’t correct. The Kutta–Joukowski theorem is a physical principle and it requires ETT in non-lifting flows. I have explained that in detail. Dolphin (t) 13:13, 14 June 2024 (UTC)
I think we both agree that ETT is not a valid assumption for an airfoil with lift. I think we also both agree that there is a body of scholarship that does make the simplifying assumption of ETT in some specific examples. That doesn't imply to me that ETT is the usual state of affairs any more than the assumption of a spherical cow implies anything about the shape or real-world cows.
You assert that "ETT represents the flow past most solid bodies". But you have not provided a citation for that. I'm highly skeptical that this is true since just about everything moves and flutters in the wind. As Norman Smith's paper states:
...the claim that the air must traverse the curved top surface in the same time as it does the flat bottom surface...is fictional. We can quote no physical law that tells us this.
That is, in general there is no physical law that requires ETT. That's not to say it never happens, or that no physical models ever make that simplifying assumption (and when they do, the result is zero lift). Whether "most solid bodies" exhibit ETT is somewhat orthogonal to this section, so perhaps we don't need to settle that here. I do think that the recent additions and changes are a distraction and make the section less readable. I'll take a look at improving the readability while keeping your concerns about overstating the invalidity of ETT. Mr. Swordfish (talk) 16:04, 14 June 2024 (UTC)
You and I both have a thorough understanding of the Kutta–Joukowski theorem. I believe the expression “equal transit time” may be a layman’s way of saying the circulation is equal to zero; I hope we agree on that.
A small part of the problem is that ETT is not a well-defined or rigorously defined expression. To the best of my knowledge this expression is only used by authors who are repudiating this attempt at an explanation of aerodynamic lift. To the best of my knowledge none of the authors and institutions that resort to this naïve explanation of lift actually use the expression “equal transit time“; no-one actually asserts that “ETT” is true or correct. There are only people like us who assert that ETT is not correct (when applied to a body generating lift.)
Your quote from Norman Smith describes a body with “the curved top surface” and “the flat bottom surface.” He is not referring to “most solid bodies” - he is describing an airfoil!
I can supply a quotation from Anderson’s “Fundamentals of Aerodynamics” that will help on this topic. I expect to get access to my copy of Anderson within 7 days. Dolphin (t) 14:30, 15 June 2024 (UTC)
Agree that ETT is not well defined, and that it doesn't appear to be used other than by those repudiating it. Searching for the phrase (or even the word "equal") on my user page collection of works presenting ETT as correct only finds that in the references, not the actual works themselves. Similarly, the obstruction explanation is sometimes derisively referred to as "hump theory" but it's proponents don't use that phrase.
A typical turn of phrase is "The air moving on the top has to travel a greater distance in the same amount of time." or "Air flowing over the top has a greater distance to travel in the same time; that's why it flows faster."
I don't know that the expression “equal transit time” is a layman’s way of saying the circulation is equal to zero, since I would surmize that those advancing the idea probably don't know what circulation is. That said, here's a source basically confirming that ETT and Γ=0 are the same idea.
Regarding whether most flows around solid objects exhibit ETT, if that were true than vortex shedding and Vortex-induced vibration would not pose problems for engineers to overcome.

References

  1. Flight Physics: Essentials of Aeronautical Disciplines and Technology, with Historical Notes (1st ed.). Springer. 2009. p. 144. ISBN 1-4020-8663-6. In conclusion, there is no possibility that the particles passing above and below the aerofoil would arrive simultaneously at the tail, except for the case that there is no circulation around the section – in this case, there is no lift on it.

Mr. Swordfish (talk) 16:20, 15 June 2024 (UTC)

Edits finished. Hopefully that addresses the concerns above. Mr. Swordfish (talk) 16:36, 14 June 2024 (UTC)
Your recent edit to the article is an acceptable alternative to my edits. Thank you for making those changes.
The article now avoids giving readers the impression that ETT is inherently false. Hopefully readers can now see that the only falsehood is suggesting ETT exists in the flow around a lifting body. Dolphin (t) 14:46, 15 June 2024 (UTC)
Thanks for the reference to “Flight Physics:Essentials ...” I was not aware of that publication. It looks like it might be essential!
Vortex induced vibrations are an oscillatory phenomenon. They become a problem in structures that have inadequate stiffness or inadequate damping. In our article on lift we are talking about steady flows with zero viscous effects, or only minor viscous effects. We use a reference frame attached to the airfoil or solid body so the consequences of oscillations of a solid body are way beyond the level of analysis we are using in this article, and related articles.
Could it be that after half a lifetime of believing that ETT is false, the work of the devil, it will take a major change of direction to accept that there is nothing false or distasteful about ETT? Could that be why you are finding reasons to deny the inevitability of flows in which circulation is zero, ETT prevails and lift is zero? Dolphin (t) 03:46, 16 June 2024 (UTC)
It's not that I don't believe lift can be zero (and that implies ETT). I just don't think it occurs as often as you seem to think it does i.e. 99% of the time a solid body is immersed in a moving fluid. That's because almost all real world objects are not perfectly symmetrical and that implies an asymmetrical air flow hence non-zero circulation.
Stated another way, ETT is not a valid assumption in general. If you assume ETT, you will get zero lift. I don't have a cite for this and I am willing to consider evidence to the contrary, but real-world airflows around solid objects with zero circulation are the exception rather than the rule. For instance, consider a symmetrical airfoil in a steady flow - it is well established that the lift varies by the angle of attack. For the special case of zero AOA, the lift is zero and ETT occurs (in this simple 2-d model). For all the other values there is lift, circulation is non-zero, and ETT is false. In mathematical terms, the set of values for which ETT holds has measure zero. That's about as rare as you can get without it being never.
Perhaps there is some area of aerodynamic research that assumes ETT or decides that lift is small enough that lift is negligible - many treatments ignore viscosity, or compressibility for example - I'm not aware of any that assume zero lift, but maybe there are. Let me know if you know of any. Mr. Swordfish (talk) 13:00, 16 June 2024 (UTC)
There are several elements of your edit on which I can comment but at present I only have time for one. I will comment on others later.
You write about “real-world solid objects with zero circulation ...” Then you make a sneaky gear change and write about “a symmetrical airfoil ...” The two are very, very different in aerodynamics so your gear change doesn’t go unnoticed. Yes, a well-designed airfoil will produce lift (and lift coefficient and circulation) that varies approximately linearly with angle of attack. The feature of a well-designed airfoil that yields this desirable property is the sharp trailing edge. Clancy’s book Aerodynamics addresses the role of the sharp trailing edge and the way it causes vortex shedding to adjust the strength of the bound vortex to maintain the Kutta condition. I don’t have Clancy with me but I think it is Section 4.5 and/or 4.8 that contains good explanatory diagrams.
In the absence of a sharp trailing edge, any change in orientation of a body is not accompanied by a change in lift (or lift coefficient or circulation.) For example, a cylinder with elliptical cross section, immersed in a flow produces little or no lift; altering the orientation of the cylinder doesn’t produce much change. What lift might be produced is due to asymmetric boundary layers and separated flow, rather than due to the primary flow predicted using an inviscid fluid. If a body doesn’t have a sharp trailing edge, and the orientation of that body is changed, the fluid flow adjusts itself so that circulation remains zero. Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge. Airfoils have sharp trailing edges, but real-world solid objects don’t. That is why the only circulation and lift that are observed on bodies without sharp trailing edges is the small amount caused by asymmetric boundary layers on the two sides of the body, separated flow and possibly other minor viscous effects.
Scientists and engineers have to work hard to generate circulation and lift. Typically they use airfoils with thin, sharp trailing edges even though this feature is structurally weak and vulnerable. Flowing fluids are uncooperative - as they flow around bodies their natural state is doing so with zero circulation. Any change in orientation of a real-world solid body causes the fluid to change its flow pattern to avoid circulation developing. If it were not so, aircraft designers would use wings with thick, generously rounded trailing edges so they could get more fuel into the wings, use deeper and lighter spars, and have more room into which to retract the undercarriage. Dolphin (t) 16:18, 16 June 2024 (UTC)
On the matter of the sharp trailing edge there is a very useful quotation by George Batchelor in the short article Trailing edge.
There is also a useful quotation by Richard von Mises at Airfoil, reference number 4. Dolphin (t) 00:38, 17 June 2024 (UTC)
The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation. Picture the wind blowing around such a body, and then the wind changes direction. Imagine that this change causes a circulation to begin in the flow. This circulation causes a lift force to act on the solid body. Newton’s 3rd law tells us that an identical lift force acts on the flowing air. When a fluid that is free to flow or change shape is subjected to a force or pressure it responds in whatever way will cause that force to diminish. Consequently the lift force on the air flowing around the solid body causes the streamlines, velocities and pressures to change to diminish the circulation that has just begun. This process can be expected to continue until all circulation has been eliminated. Only then has equilibrium been achieved within the flow pattern around the body.
Any residual circulation and lift is not related to the primary flow as would exist in a geometrically similar situation but with an inviscid fluid. It is related to the secondary flow caused by viscous effects such as flow separation. Any residual lift is still accompanied by the original drag force. The lift to drag ratio is so small that this solid body doesn’t qualify as an airfoil. I believe this is an explanation for the operation of oddly shaped lifting bodies which glide without conventional wings. Dolphin (t) 05:22, 17 June 2024 (UTC)
I'm continuing this discussion since I think I may learn something. I'm not trying to be "sneaky", just trying to understand what evidence there is that zero-circulation/zero-lift/ETT is the usual or normal state of affairs rather than a rare exception.
>Circulation greater than zero requires the Kutta condition, and the Kutta condition requires a feature resembling a sharp trailing edge.\
Agree that Kutta condition requires a sharp trailing edge, because without one it's not obvious where the rear stagnation point occurs. And without that it's not clear how much circulation to apply to model the fluid re-joining at the rear stagnation point. But you don't need a sharp trailing edge to have an asymmetrical airflow with non-zero circulation, you just can't apply the Kutta contidion. As Gale Craig states, (paraphrasing) you don't need an airfoil shape to get lift, as anyone who has ever handled a sheet of plywood in the wind knows. Of course, if you want enough lift to fly a plane of propel a sailboat, you'll want something with more lift than a non-arifoil can provide. That doesn't mean only airfoils with sharp trailing edges can generate lift.
I have sailed boats with rudders that have a rounded trailing edge. Performance is sub-optimal, but the rudder most definitely provides enough lift to steer the boat. When I look at leaves on trees or flags on a flagpole in the wind, they never settle down into an equilibrium of zero lift as you describe above. Spinning balls have lift, as any tennis player understands. Here in the US, there's a baseball pitch called the knuckleball where the ball is thrown with a little spin as possible, with the effect that it's impossible to predict which direction the lift will take the ball making it very hard to hit. So, my experience is quite at odds with your assertions.
You say that "The conventional wisdom is that fluid flow around a real-world solid body experiences zero circulation." but don't provide anything to back that up. Along with your 99% figure, I would need some more to go on than your assertion.
Agree that my examples above are anecdotal or original research. Here's an interesting treatment of bluff bodies which seems to be in conflict with your assertion that Circulation greater than zero requires the Kutta condition...
For bluff bodies, the interest is usually in the drag on that body, mainly because experiments have found that drag is the dominant force. This observation, however, does not imply that bluff bodies cannot produce lift because many do. Nevertheless, examining just the drag characteristics of such bodies is convenient in the first instance. Furthermore, bluff bodies may also produce pitching moments, which sometimes need to be known for certain types of engineering work, e.g., to determine torsional loads.
Mr. Swordfish (talk) 13:56, 17 June 2024 (UTC)
Here's an excerpt from another paper BLUFF-BODY AERODYNAMICS
Bluff bodies are obviously also subjected to forces in the across-wind direction and to
moments around the various axes due to non-symmetries of the pressure distribution on their
surface. Therefore, these loads depend fundamentally both of the body shape and on the
orientation of the incoming freestream. Particularly in the two-dimensional case, the force
component in the across-wind direction is often called lift force, in analogy to the
corresponding force acting on an aeronautical wing section (airfoil).
(elision of details about the starting vortex and consequential circulation around an arifoil)
Coming back to bluff bodies, the above described mechanism does not apply in all its
details, particularly because the boundary layer cannot remain attached to their surface even
after the end of the initial transient. However, if the body is sufficiently elongated (like an
ellipse), a starting vortex is shed anyway (even if not as strong as that of an airfoil), and the
asymmetry of the final flow configuration for non-symmetrical wind orientations may be
sufficient for producing significant lateral forces.
Seems to me that if it were the case that almost all bluff bodies experience zero lift the paper would say that at some point. Mr. Swordfish (talk) 14:32, 17 June 2024 (UTC)
One of the frustrating aspects of discussing this subject is the variation in meaning given to the word “airfoil”. On these Talk pages I see the word used with three different meanings:
  1. A two-dimensional shape that can be employed in three-dimensional bodies to generate lift. For example, the shape known as NACA 2412 is an airfoil section commonly used for the wings of low-speed aircraft.
  2. A three-dimensional body that generates at least a little lift. Some Users point to an irregular body or a sheet of plywood or a sycamore seed and, noting that it experiences a small lift force, say “see, it is an airfoil!”
  3. A three-dimensional body that, over a usable range of angle of attack, is capable of generating significantly more lift than drag. With this meaning, airfoils are manmade structures that have the generation of lift as their primary purpose. Airfoils are carefully designed and manufactured structures to ensure the lift-to-drag ratio is high enough to achieve its intended purpose.
Misplaced Pages’s current definition of airfoil closely matches No 3 above. Airfoil says:
When the wind is obstructed by an object such as a flat plate, a building, or the deck of a bridge, the object will experience drag and also an aerodynamic force perpendicular to the wind. This does not mean the object qualifies as an airfoil. Airfoils are highly-efficient lifting shapes, able to generate more lift than similarly sized flat plates of the same area, and able to generate lift with significantly less drag. Airfoils are used in the design of aircraft, propellers, rotor blades, wind turbines and other applications of aeronautical engineering
The layman imagines that the essential feature of an airfoil (meaning No 3) is its generously rounded leading edge, or its curved surface. In fact it is the trailing edge. That is partly the explanation of why a flat sheet of plywood will experience lift in a flow of air - it has a sharp trailing edge.
Since the days of Joukowski and Kutta, mathematicians and physicists have been able to model the flow of an inviscid fluid around suitable geometric shapes. With a sharp trailing edge it is possible to determine the lift and pitching moment on the shapes. Tests on real models of wings in wind tunnels show there is close agreement between the math and the real world for these shapes with sharp trailing edges. For bodies without a sharp trailing edge, the math shows that an inviscid fluid imparts no lift or pitching moment to the body.
Wind tunnel tests on bodies without sharp trailing edges, and anecdotal evidence, show that these bodies can experience a little lift. This does not mean they qualify as airfoils under meaning No 3 above. Engineering, and most science, have little interest in these bodies. What lift they develop is not due to airfoil action - exploiting the Kutta condition to generate lift. It is due solely to viscous effects such as flow separation. These bodies, at best, have a very low lift-to-drag ratio. Little is written about them in mainstream science or engineering publications. This type of lift has little or no engineering application.
We know that eating a tablespoon of salt a day won’t cure cancer, but it is probably impossible to find a reliable published source that confirms eating a tablespoon of salt a day won’t cure cancer! Similarly it is probably impossible to find a reliable published source that confirms that no bluff body has ever been found that is capable of a high lift-to-drag ratio.
We use the Kutta condition to determine, mathematically, the circulation around a 2-D shape with a sharp trailing edge edge. There is no similar model, theory or equation to determine circulation around a 2-D shape with no sharp trailing edge. I suspect that wind tunnel tests would not show a usable relationship because, being reliant entirely on viscous effects, the results would be strongly influenced by the surface conditions of each model being used - roughness, smoothness, manufacturing imperfections etc.
When I say that bodies without sharp trailing edges do not generate circulation in fluid flows around them, I am speaking as an aerodynamicist applying the model of the inviscid fluid. There is no doubt that my statement is true for inviscid flows, which admittedly are fictitious, but this is usually a good, simple guide to the reality of high Reynolds number flows. When you say that all bodies in a fluid flow experience viscous forces and these forces will provide at least a very small amount of circulation that cannot be eliminated by the flow pattern adjusting itself you are possibly speaking as a scientist focussed on observing the complex realities of the real world. You aren’t able to determine how much circulation there will be, or say exactly how that circulation is sustained. What circulation exists is small and I say it is zero. You possibly describe the same situation by saying circulation is not zero. That might be as close to consensus as we can hope to reach. Dolphin (t) 15:39, 17 June 2024 (UTC)
Agree that I am sometimes a bit loose with the terminology re: airfoil. One other possible avenue of miscommunication here is that when I see the word "lift" in this context I think of the definition used in the first sentence of the article:
When a fluid flows around an object, the fluid exerts a force on the object. Lift is the component of this force that is perpendicular to the oncoming flow direction.
and as a mathematician rather than an aerodynamic engineer lift=0 means actually zero, as opposed to "too small to be useful or significant." One of the arts of engineering is to figure out what things can be ignored, and for most non-airfoil applications the fact that there is some component of the aerodynamic force perpendicular to the airflow is negligible. I'm sure that there are many situations where we would agree that whatever small amount of lift might be present, it's too small to matter so let's assume it is zero. This would imply ETT in that situation.
Other situations I wouldn't agree that it's too small to matter, for instance, a leaf on a tree in a breeze - the leaf repeatedly flutters back and forth in a direction perpendicular to the airflow and this implies to me that there is some force making it move that way and the obvious one is that there is some non-zero component of force transverse to the airflow. I would call that "lift" according to the definition above. But since I doubt either of us will be hired as an engineer to design tree leaves any time soon we can leave it there. Mr. Swordfish (talk) 17:56, 17 June 2024 (UTC)
Thanks. I agree with most, if not all, of what you have written. I now realise that the concepts of streamlines, time slices, circulation and ETT are all concepts that rely on steady flow. When we are talking about a turbulent wake, separated flow, oscillatory flow, the erratic dancing of the leaves and branches of a tree, we can’t claim the protection offered by retreating to steady flow. Debating about streamlines, time slices and ETT in a non-steady flow is deeply flawed.
The dancing of leaves on a tree is definitely caused by the interaction of aerodynamic forces and elastic forces within the highly flexible structures of a tree. This kind of motion could be caused entirely by drag, so I’m not persuaded that the dancing motion of a leaf necessarily shows the presence of lift.
The concepts of lift and drag rely on knowing the direction of the local velocity of the fluid. The air moving through the branches and leaves of a tree is highly disorganised and the velocity at each point is changing rapidly so it is probably true to say that while we can possibly identify aerodynamic forces acting on branches and leaves, the concepts of a drag component and a lift component are not applicable. The distinction between a lift component and a drag component seems to be reliant on steady flow, and flow in which the speed and direction at one point is almost identical to the speed and direction at all nearby points.
The Kutta-Joukowski theorem is remarkably similar to Newton’s 1st and 2nd laws. Scientists and engineers say Newton’s laws are valid. Perhaps a mathematician and philosopher might say Newton’s 1st law is redundant because there is no such thing as a body whose acceleration is truly zero; and no such thing as a body experiencing a net force that is truly zero. Dolphin (t) 00:30, 18 June 2024 (UTC)
In my edit dated 15 June 2024 (14:30) I wrote “I can supply a quotation from Anderson’s Fundamentals of Aerodynamics that will help on this topic.” See the diff. In section 3.16 Anderson writes about the Kutta-Joukowski theorem:

"Although the result given by the equation L = ρ V Γ {\displaystyle L^{\prime }=\rho _{\infty }V_{\infty }\Gamma } was derived for a circular cylinder, it applies in general to cylindrical bodies of arbitrary cross section."

This confirms that the Kutta-Joukowski theorem is not confined to airfoils. It applies to all cylindrical bodies regardless of their cross sectional shape. If a cylinder of arbitrary cross section causes no circulation in the flow in which it is immersed the cylinder will experience no lift.
It is not too great a leap to say that, just as airfoils are associated with the Kutta condition to explain when they will generate lift, and when they won’t, cylindrical bodies of arbitrary cross section also rely on a feature resembling a sharp edge to obtain a well-defined lift. If these bodies of arbitrary cross section experience lift in the absence of a sharp edge, it is due to viscous effects such as flow separation and asymmetric boundary layers, rather than due to airfoil action.
My mention of a well-defined lift is from "sharp trailing edge to obtain a well-defined lift" as written by Richard von Mises. See citation No. 4 in Airfoil. Dolphin (t) 12:44, 30 June 2024 (UTC)
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