Talk:Inductor: Difference between revisions

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	==Straight wire conductor formula==
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	Straight wire conductor formula for inductance contradicts itself.. :/ <span style="font-size: smaller;" class="autosigned">—Preceding ] comment added by ] (]) 23:24, 4 November 2009 (UTC)</span><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->
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	== '''Units of inductor formulas''' ==
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	The units of many of the inductor formulas do not work out as they are currently written. The first and last appear to work out, but the units of the short air core cylindrical coil equation for example gives you micro Henries = inches. My guess is that the equations are correct, but are missing some units hidden in the constants. These should be explicitly shown.
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	Also the ] page, and the ] page should have their equations coordinated. They are giving very different equations.] (]) 17:16, 19 August 2010 (UTC)
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	== '''Effect of one inductor on another''' ==
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	If there are two inductors connected in series in the same circuit and their mutual inductance is 0,can one inductor affect the flux through the other inductor in any way?-Subhash
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	: That's not a homework question, is it? — ] 13:17, 7 August 2006 (UTC)

	Please give me a valid answer.I'm stuck up in a controversy related to this in the classroom and I want to know the fact.–Subhash
	:The question isn't really phrased "tightly" enough to answer. If the two inductors share (essentially) no flux (and so have essentially no mutual inductance), then they are independent components. The total inductance is the sum of the two individual inductors and the total impedance is the vector sum of the two individual impedances.

	:However, by adding its own contribution of L, R, and C into the series circuit, the second inductor clearly affects the flux developed in the first inductor and vice-versa; remove the second inductor and the flux in the first inductor '''will''' change (and vice-versa).

	:] 13:21, 8 August 2006 (UTC)

	Thank you for answering my question.Considering a pure inductor, what if the second inductor's current is suddenly diverted by the means of a switch when they(Both the inductors) have already reached(considering DC) steady state?That is, if the second inductor is somehow thrown out of the circuit after reaching steady state ,does the first inductor's flux or current get affected in some way(Considering 0 mutual inductance)?

	:Well, in the case of ideal inductors, your question isn't meaningful because, when connected to DC, our ideal, resistance-free inductors never will reach "steady state". So we'll put that case aside. ;-) For non-ideal inductors, instantly switching an inductor out of the circuit (that is, replacing it by a short circuit: a zero-resistance, zero-inductance path) will cause the remaining inductor to no longer be operating in steady-state conditions; you switched out some of the resistance in the circuit (the resistance of the non-ideal second inductor) so the current (and magnetic flux) in the remaining (first) inductor must then rise further until a new set of steady-state conditions are established.

	:Meanwhile, of course, the inductor that you instantaneously switched out of the circuit has thrown a heck of a spark as we instantaneously opened its circuit path, causing its terminal voltage to rise sharply as it tries to maintain the current flow. But tat's a topic for another discussion. ;-)

	:] 12:10, 9 August 2006 (UTC)
	::Well, it's been a while so this might be a bit sloppy, but reactance (or some function of it) depends on inductance times derivative of current. At steady state, derivative of current is zero, therefore derivative of current times inductance is zero no matter what happens to inductance number two, including switching it out of circuit, i.e. dropping it to zero. If reactance of inductor number two doesn't change, then current through whole circuit will not change, drivative is still zero, so no effect on inductor number one. ] 15:37, 9 August 2006 (UTC)

	== Coil disambiguation ==

	Just a layperson, trying to disambiguate ] -- should the currently non-existent ] be a separate article, or redirect here? or vice versa? ] 00:29 Apr 14, 2003 (UTC)

	Why is "L" the symbol for inductance? - Joseph D. Rudmin

	:The "L" was chosen after ]. --] 04:46, 30 November 2005 (UTC)

	You mean the variable (The unit is usually Henrys.)? "I" was already taken for current; "i" for the square root of -1; not sure where L came from but I suppose it makes as much sense as anything. ] 19:49, 17 Feb 2004 (UTC)

	Yes; how embarrassing! I know the difference between symbol and unit. I have corrected my question. - Joseph D. Rudmin

	----

	It's spelled ''characteristic''.

	Why did you move ] to its own article? I think it is better in the ] article with inductance as a redirect. They are essentially the same thing and should be in one article. Whether ''inductor'' or ''inductance'' I don't know, but the two belong together. That's like separating ''running'' from ''runner''. An inductor (parasitic or otherwise), and nothing else, has inductance and inductance is a property of inductors. - ] 16:58, Apr 13, 2004 (UTC)

	At the very least, equations should be moved to inductance, and actual information on construction, etc. to inductor.

	:Why? They are both about the same thing. A "parasitic inductor" is still an inductor, right? And you don't construct those. Maybe there is no such thing, and there is only "parasitic inductance"? - ] 19:32, Oct 18, 2004 (UTC)

	::I guess to a physicist, inductance is more important than an inductor, and to an EE, vice versa...? ] 14:59, 6 October 2005 (UTC)

	A '''''CHOKE'''''' is an inductor. An inductor is an electronic device. A CHOKE performs a specific task as does a TRANSFORMER, or the L in an LC circuit. The three are not necessarily interchangeable. A link from CHOKE to INDUCTOR could prove helpful. ] (]) 00:37, 11 April 2009 (UTC)MA Sala

	== ] ==		== ] ==

	I suspect that the new ] article needs to be merged with another (this one?); it certianly needs a lot of work by someone who knows what they're doing. ] (] 13:12, 30 Mar 2005 (UTC)		I suspect that the new ] article needs to be merged with another (this one?); it certianly needs a lot of work by someone who knows what they're doing. ] (] 13:12, 30 Mar 2005 (UTC)

	:No kidding; Is there much in that article that's salvagable?		:No kidding; Is there much in that article that's salvagable?
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	:] 11:47, 8 Jun 2005 (UTC)		:] 11:47, 8 Jun 2005 (UTC)

	== practical issue ==

	It would be helpful, if l - length were better explained in formulas. I think it is the gap between the two walls of the coil form.

	Also some examples of permeability ranges would be good.

	I have decided I will have to resort to pulling a book off a shelf to make even a factor of 10 approximation for a coil. <small>—Preceding ] comment added by ] (] • ]) </small><!-- Template:Unsigned -->

	it seems that some inductors use coil that is NOT electrically insulated - i.e. blank. i'd like to understand why the current will not chose the shortest path (through adjacent loops of wire, which touch one another) rather than going through every loop and building up the magnetic fied.

	:Most coils are wound with a wire with a varnish or polyurethane coating. Take and ohmmeter and you will see, it is really insulated wire. <small>—Preceding ] comment added by ] (] • ]) </small><!-- Template:Unsigned -->

	secondly, would it not be most effective (in terms of maximum henries generated per volume of space occupied) to loop the wire in TWO countered sets of loops around the same core, which build opposing magnetic fields?

	:I think you'll find that what you see as bare wire is either separated by an air gap or a thin coat of paint. The voltage between turns is not that great so you don't need much insulation. Shorted turns is a common fault in motors, etc. Multiple layer inductors do exist, but I believe they are usually wound in the same direction to avoid some bad effects. More insulation is usually required between layers. --] 13:29, 16 September 2005 (UTC)

	::Yes, winding wire as purchased is almost always insulated with a thin layer of varnish or enamel. Arnold is correct in that there are not usually many volts per turn, so a thin layer may provide enough voltage breakdown strength.
	Regarding your second point, if alternate layers were wound in opposite directions, the magnetic flux would cancel out giving ZERO inductance. In fact, this is how some non inductive resistors are wound.--] 15:44, 16 September 2005 (UTC)

	== Category? ==

	Why does ] belong to <nowiki>]</nowiki> while ] belongs to <nowiki>]</nowiki>?--] 11:55, 14 December 2005 (UTC)

	== Typo? ==

	Hi
	in the overview the word opposite appears -- do you mean opposes?

	== definition ==

	In the equation for inductance you never say that L is inductance. If it's not, you need to say what it is.
	:Symbol added. ] 20:37, 19 December 2005 (UTC)


	Inductance is the ratio of the back EMF induced to the rate of change of current.

	== Goddamn Wheeler and his inches ==

	We should present the inductance equations in the SI form, foremost, since Henry is a SI unit and hell, this is a scientific article! These "easy equations for inches" created by some guy named Wheeler, apparently, are bastardized forms of the SI ones to make the use of inches easier and convenient. Yeah yeah, I know this is the English Misplaced Pages, so yadda yadda, but we need the SI equations in there, as they're the preferred and more scientific form.

	The non-si equations could show up on a special section, even mentioning the Wheeler guy, describing how they were made up for convenience of imperial unit users, hence all the seemingly arbitrary constants. I'd do it myself, but alas, I don't have the equations, and that's also why I'm complaining. ☢ ]⌇] 21:37, 25 December 2005 (UTC)

	I completely agree with these comments - it would be nice to replace the formulae with SI equivalents. Their source should also be referenced. Finally, there is a contradiction: the formula for a coil of thickness d does not tend to the formula for a thin coil in the limit d->0. As someone else has commented, if these are approximate formulae, their regions of applicability should be stated. ] (]) 09:43, 18 May 2010 (UTC)
	:: And here it is nearly 5 years later and no apostles of SI have stirred themselves to post metric versions of the inductance formulas. Scientist use whatever system of units is handy, and if there isn't one, they'll make their own units. --] (]) 19:59, 19 August 2010 (UTC)

	:::For every devine's sake! The whole world uses the SI! Or would it be ok to change all inches to seamiles? Or imperial miles? Foot? Feet? I don't care if a farmer in the most outer long forgotten corner called the USA uses the imperial system! Sorry for my rage, but this is not America, nor the uk, this is a worldwide encyclopedia. <span style="font-size: smaller;" class="autosigned">— Preceding ] comment added by ] (]) 13:29, 28 September 2011 (UTC)</span><!-- Template:Unsigned IP --> <!--Autosigned by SineBot-->
	::::You shoulnd't make a system of measure your religion. The choices are all arbitrary, no matter how much significance you attach to the distance to the King's nose or how many wavelengths of krypton light to use. --] (]) 14:34, 23 December 2011 (UTC)
	::::: Actually they are not arbitrary, they are international standards. That they became international standards was abitrary, but that is something decided long in the past. SI units now stand out uniquely as the lingua franca of engineering discourse. The presence of inches on this page is an embarassment.] (]) 13:10, 9 January 2012 (UTC)

	The issue here is not whether to use SI or some other unit system. The real issue is YOU SHOULD NOT MAKE EQUATIONS DEPEND ON THE CHOICE OF UNITS. (Sorry for shouting.) I've studied university-level physics in three countries, and only in the U.S. have I come across shit like "The area of a triangle is given by A = 216wh, where A is area in square inches, w is width in feet, and h is height in yards". In any other country, the formula is simply given as "A = w*h/2, where A is area, w is with and h is height" and you are free to use whatever units you like.

	If you take the (correct) formula <math>L=\frac{\mu_0KN^2A}{l}</math> and use either inches or meters, you get the same answer. You can also deduce the unit of L from the units you input. If you take the (incorrect) formula <math>L=\frac{r^2N^2}{8r+11d}</math> it doesn't really matter what units you use. L will come out in units of length, not inductance. It is possible that the original reference is correct (I haven't checked) but whoever copied it into the article failed to include the symbol <math>mu_0</math>. In that case, the formula will work regardless of unit system. Or it could be that these formulae only work with a carefully chosen set of units, in which case they are worthless and need to be converted to a useable form. ] (]) 15:13, 13 January 2012 (UTC)

	== "j is in ohms" ==
	It says in the text "The impedance of an inductor (inductive reactance) is then given by:", then an expression, and then it's stated that "j is in ohms". Is this really true? Isn't j the imaginary unit, such that j^2 = -1, and isn't that unit always dimensionless? I think this is just a typo in the article, but I thought it best to seek consensus before editing, anyway. --] 08:24, 24 February 2006 (UTC)

	:] can be a complex number. Take a look at the article for some more insight on that statement. ☢ ]<span style="font-size:120%">⌇</span>] 08:46, 24 February 2006 (UTC)

	:: But the imaginary number is not in ohms. It's a number. Does the article mean "j ohms"? — ] 16:52, 24 February 2006 (UTC)

	::: Yes, imaginary numbers have dimensions as well. It's always the same dimension as the real component. I suppose you can debate whether or not they're real ohms, but then we are talking about an imaginary number, so I think that makes them imaginary ohms rather than real ohms by definition.

	:::: No, imaginary numbers do not have any dimension. The real component has no dimension, the imaginary component has no dimension. The sum has no dimension. Numbers are always just numbers. Constants, however, may have dimensions. ] (]) 13:14, 9 January 2012 (UTC)

	::: I can't find what you're talking about in the article, so I'll just explain briefly. For a given frequency, an inductor will oppose the flow of alternating current similar to how a resistor would. Whatever the formula was, it calculates this resistance. (and it's important to note that, whatever the value is, it changes when the frequency of the AC changes) It differs from real resistance in the way in which two resistances in series add together. If you add together two inductance-style resistances, it's the same as adding together two resistance-style resistances, but when you add one of each, they add differently. The way it works out is that you consider the resistor-style resistance a real component of the total resistance, and the inductance-style resistance an imaginary component, then add them together (which in this simple case is simply combining 10 ohms with 10 imaginary ohms to end up with a ] like 10 + 10i ohms) and you calculate the effective resistance by finding the ] of this number (which is about 14 ohms in this case). Interestingly, you can do the same with capacitors, but it is convention to assign capacitors negative imaginary values, since when capacitance-style resistance is added to inductance-style resistance, the two cancel eachother out.

	::: I suppose it might be nice to put that in the article somewhere, but my writing style is so unencyclopedic. "Inductance-style resistance" isn't a real term -- I just made it up -- and all of this information is coming from a college textbook someone gave me which I threw away because I didn't like it, and thus I can't provide references. -- ] (]) 21:28, 18 July 2008 (UTC)

	'i' is the ''mathematical'' symbol used for imaginary numbers. However, in electrical/ electronic context i or I is the symbol for ''current''. Therefore j is used in place of i/I in electronic calculations. To save confusion between I current and i the 'imaginary root' of -1)

	Thus, 10 + 10i ohms should really be written, for electronics use, as 10 + 10'''j''' ohms
	--] (]) 12:13, 24 October 2009 (UTC)

	j is unitless, the unit for reactance, X, is in ohms. That way, when you say Z = R + jX it makes sense. <span style="font-size: smaller;" class="autosigned">—Preceding ] comment added by ] (]) 00:56, 25 October 2009 (UTC)</span><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->

	== Hydraulic Model ==

	Sureley, a transformer could be modelled hydralically by having a pair of differently-sized "turbines" hooked together mechanically - running on the same shaft. One could even connect the two tubine shafts with a slippery ] to model transformer losses.

	] 03:19, 25 May 2006 (UTC)

	Your idea is a great one but magnifying the voltage through induction is much more easier as well as efficient because there are no moving parts involved in a transformer.Besides when dealing with voltages as high as 750KV it is never safe to convert the electrical energy into mechanical energy.] 04:53, 15 August 2006 (UTC)

	:Any way of modeling a transformer would be stretching the hydraulic analogy too far. Removed. ] 17:05, 19 August 2006 (UTC)
	:: I'd like to remove the hydraulic model altogether - it seems contrived, and the effort you spend puzzling out the analog is better spent puzzling out how a magnetic field builds and collapses. --] (]) 17:00, 19 August 2010 (UTC)
	:::Well said. I second the motion to remove the hydraulic model altogether. ] (]) 17:33, 19 August 2010 (UTC)
	:::: It's gone now. It seemed gratuitiously complex, since the mass of the flowing fluid would be sufficient, if you defind "mass rate of flow" to be like "current" and "pressure" to be like "voltage" and ignore the quadratic pressure drops across orifices....etc. Of course that doesn't let you explain mutual inductance. Some editors really like hydraulic analogies...--] (]) 18:23, 19 August 2010 (UTC)


	== Nutshell ==

	So... in essence, an inductor tries to keep the current flowing at a constant speed...? (Please respond on my talk page.) ] 23:02, 15 September 2006 (UTC)

	:I would rather say that an inductor keeps the current constant when the voltage at its connections is zero. To change the current you must apply a voltage. The other way: When you "tamper" with the connections, it creates voltages to keep the current going. ] 14:58, 10 October 2006 (UTC)

	== Help? ==

	What's the average inductance of an inductor? Like, 1H, 5H? What would a 1H and a 5H inductor be used for? (Please respond on my talk page if you must.) ] 18:29, 9 November 2006 (UTC)


	There is no "average" inductance since the inductor value is always chosen depending on the task it is needed to complete. Since all tasks are different each task will have a different-sized inductor. Furthermore, inductors are usually very easy and cheap to make (just a wound loop of wire that doesn't even always need a core) so there is no need usually to standardize sizes. That being said, it is unusual to have one over 1 Henry in size. More likely you will be dealing with millihenries or microhenries. <small>—Preceding ] comment added by ] (]) 21:08, 17 December 2007 (UTC)</small><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->

	== Q Calculation ==

	How about some way to calculate the Q of an inductor? The book "Reference Data For Radio Engineers" contains a graph that will give the Q for some solenoidal inductors. I was looking to calculate it or an air cored torroid, came here but NADA! Anybody know how to do this? (Yes, Iknow it's difficult!)

	:The Q is simply L/R (ratio of inductance in Henry and (DC) resistance in Ohm). Q depends on the frequency, so an inductor may have a different Q at a different frequency. The frequency dependent part can be major factor with, for example, ferrite core inductors. It is, if my memory serves me well, almost a non-issue in air-core inductors (the magnetic properties of ] are very small compared to those of ferrite materials; note that the ] incorrectly states that Oxygen is only ] is liquid and solid form - some physical gas detectors do in fact use the paramagnetism of oxygen). --] 16:54, 4 March 2007 (UTC)

	::Q depends on frequency???. How so? Does the L depend on frequency? The R? If so, then neither is an L or an R. Yes, ''reactance'' depends on frequency but not L or R. ] 04:21, 5 March 2007 (UTC)

	== Formulas and approximations ==

	As far as I recall, the formulas for conculating some inductance from some coil diemnsions are just approximations. With "typical" parameters, a lucky coil builder may get reasonably close results when winding his coil in real life, but he may appear to be less lucky when he designs his special 1.3 turn coil, whose parameters he verified with the mentioned formulas. Perhaps it should be noted which formulas are approximations and under which circumstances they provide reasonable results. Unfortunately, I have only vague memories on this topic, so I cannot help myself :-( --] 15:33, 4 March 2007 (UTC)

	== Formulae units ==

	Is it really necessary to have non-SI versions of some of the inductance "formulae"? This isn't standard practice on WP, and seems somewhat arbitrary. If people are working in imperial units, they can easily convert to SI before applying these equations. ] 18:25, 17 June 2007 (UTC)

	: No, we don't need these at all. Only commonly-used equations. — ] 00:20, 18 June 2007 (UTC)

	== Stored Energy ==

	It'd be super-awesome if someone could make the section on stored energy look similar to the section on stored energy in the article about ]. Over there, I think it makes it easy to understand why the equation is what it is, whereas here, I'm left wondering why it is what it is. It's very symmetrical, so I'm sure it's correct, I'm just having a difficult time understanding how one determines "the amount of work required to establish the current through the inductor" which would be awesome information to have. -- ] (]) 21:36, 18 July 2008 (UTC)

	: I think the key to understanding this is to turn around the definition of a henry. The standard definition is "an inductor with an inductance of 1 henry produces an EMF of 1 volt when the current through the inductor changes at the rate of 1 ampere per second." In equation form this is H = V / ΔI, indicating that the value assigned to inductance increases when the EMF voltage increases, and decreases when the current required to create this voltage increases. To make this easier to understand, just rearrange it to ΔI = V / H, which indicates that the change in current increases with applied voltage, but decreases with increased inductance. This makes the whole issue of inductance a lot easier to understand. Want to know what happens when you apply 5 volts to a 1 mH inductor? Well, 5 / 0.001 = 5000, so the current increases at a rate of 5000 amperes per second when 5 volts is applied to this inductor, at least until your power supply fails. Needless to say, such voltage is always applied to such inductors for very short periods of time, or via resistors which will cause the applied voltage to decrease as the current increases.

	: So anyway, imagine you apply one volt to an inductor of one henry. Over time you will see a linear increase in current, rising to one ampere after one second, and two amperes after two seconds. Since power equals voltage times current, we can calculate the power going into the inductor at any moment. At one second it is one watt, at two seconds it is two watts, and this can be integrated to end up with the equation in the article. If you don't want to integrate, just draw a graph (linear graphs are easy) and shade the area under the line to represent the stored energy. After one second, you have half a shaded square. After two seconds, you have two shaded squares. After three seconds, you have 4.5 shaded squares. All which are the same values given by the formula in the article.

	: I suppose this too would be nice for the article, but I kind of just made it all up. The way that calculus is written makes absolutely no sense to me, so I've kind of had to figure out stuff like this on my own. I can't seem to find a reference that doesn't use standard calculus notation and so I'm not sure anything actually agrees with me. All I know is that when you integrate y = b * x, you end up with 0.5 * b * x ^ 2, which leads to the equation in the article. -- ] (]) 02:57, 21 July 2008 (UTC)

	== current flow of an inductor ==

	equation for current flow of an inductor at any given time passed the point at witch voltage was applied.
	Finding the current flowing in an inductor at any given time past when voltage was applied.
	:<math>Amps = \left ( \frac{Vsource}{Rseries} \right ) * \left ( 1.0 - e ^\left ( -Time * \frac{Rseries}{inductance} \right ) \right )</math>
	<math>e</math> is inverse natural log or normally <math>e^x</math> on most calculators.
	This was removed for a unknown reason. I believe it to be common knowledge among ET and EE people so it was not cited. ] (]) 22:16, 31 July 2008 (UTC)

	:For a start, "amps" isn't a quantity, it's a unit! What's more the maths was badly formatted, and the more general formula is:

	::<math>\ I(t) = I_0 ( 1 - e^{-\frac{tR}{L}})</math>

	:This belongs with the material in the "In electric circuits", but it needs working into the existing text. I will do that shortly. ]<sup>(]\|])</sup> 22:33, 31 July 2008 (UTC)

	== cylindrical coil inductance formula is wrong ==

	the formula does not include K the Nagaoka coefficient (im assuming they are using nagaoka's formula for single layer coil inductance), the formula should be:

	::<math>L=\frac{\mu_0KN^2A}{l}</math>

	<math>K</math> and <math>\mu_r</math> are not the same afaik.

	: the Nagaoka coefficient offers a small correction; it is defined as K=1/(1 +0.9 r/a -0.02 (r/a)²) where '''r''' is the radius of the coil and '''a''' is the coil length. found after some digging at <ref>http://www.freepatentsonline.com/5903242.pdf</ref> -- ] (]) 21:27, 21 March 2010 (UTC)


	Shouldn't this equation use <math>\mu_r</math> as well as K? this represents the situation where the core material is ferromagnetic.] (]) 22:41, 18 August 2010 (UTC)

	I retract my statement, looking at the page for inductance, it is clear the situation is not as simple as that and going into more depth would just confuse matters more. However it should be made clear that the equation gives the inductance of a solenoid in air, not one with a ferromagnetic core. ] (]) 16:30, 19 August 2010 (UTC)

	== Merge ] into this article? ==

	The stuff in ] looks mostly either redundant or irrelevant. --] (]) 19:20, 22 September 2008 (UTC)

	:I'm surprised such an article exists. It is the same thing as an inductor. Maybe it can have its own section on this page. Its list of Core examples is useful though. ] 23:52, 23 September 2008 (UTC)

	::I agree, it should be merged into this article. --<font color="blue">]</font><sup>''<small>]</small>''</sup> 05:19, 24 September 2008 (UTC)
	:::NOT AGREE ! Electromagnetic coil → ]
	:::Inductor → ]
	:::clean up the articles.--] (]) 09:09, 6 November 2008 (UTC)
	:::I do not agree <span style="font-size: smaller;" class="autosigned">—Preceding ] comment added by ] (]) 03:52, 2 October 2010 (UTC)</span><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->
	The articles ], ] and to some extent ] all refer (as far as I can see) to the same object, an inductor. I do not understand the reference to the two German articles, one about a component (a coil) and one about a physical phenomenon and basic unit (Inductance). --] (]) 10:48, 27 February 2009 (UTC)

	:An ] is a type of ], combined with a vibrating interrupter switch. Clearly not a simple inductor. The "]" was (according to the article) a communications system, referring to the amplifier as well as the wire loop. In my view ] could go either way; its a specialized type of inductor, perhaps different enough from other inductors to merit its own article. However ] is a mere generic term for a coil of wire, that could refer to an inductor or a ] or perhaps a ], so I feel it's too broad to have its own article and should be covered in those existing articles. Maybe the German term "''spule''" has a more specific meaning, but in English it is simply a coil of wire. --<font color="blue">]</font><sup>''<small>]</small>''</sup> 19:08, 27 February 2009 (UTC)<br /><br />
	:Concur with Chetvorno, ] is more than a simple ]. This specialized device merits its own page. The merge sugestion has been removed from both articles. ] (]) 19:14, 1 March 2009 (UTC)

	:Induction loop is an independent topic about a communications device and should not be merged with inductor. ] (]) 13:55, 24 June 2009 (UTC)

	I think the reason people try to merge different things into one is an absence of understanding the difference, which is the HUGE GAP between a "perfect mathematical inductor", defined by the familiar differential equation and the REAL devices, working by absolutely different principles. BTW, most electronics articles refer to simplifies (not to say stupidified) mathematical models, while absolutely ignoring the real world components and their application in real world circuits. No fun... :( ] (]) 13:05, 5 May 2009 (UTC)

	I think it's clear that the merger proposal should be removed, because inductor is not a coil and vice versa. ] (]) 13:44, 5 May 2009 (UTC)

	:It seems to me that ]'s issue is irrelevant to whether ] should be merged. All inductors depart from their ideal circuit models due to resistance, ], ], ], ], etc. This article deals with both the ideal circuit model and construction of real inductors. I agree it doesn't include enough about the above real world effects, but this should be fixed by adding to this article. --<font color="blue">]</font><sup>''<small>]</small>''</sup> 17:08, 11 June 2009 (UTC)

	In relation to merging the article ] with the article inductor, leaving aside the technical differences discussed above, as a user I feel it should not be merged on the basis of common usage - the term choke is widely used in engineering and industry for this type of device, and my personal view is that it warrants its own article despite being part of a wider group of technically similar devices. <span style="font-size: smaller;" class="autosigned">—Preceding ] comment added by ] (]) 11:18, 5 July 2009 (UTC)</span><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->

	Absolutely merge "choke" into "inductor". A choke is simply another term for inductor, and is somewhat archaic. It is what condenser is to capacitor. The content should be merged into inductor. As for "electromagnetic coil", that is a description, not a name. ] (]) 20:08, 15 February 2010 (UTC)

	''A choke is a principle involving an inductor to serve a purpose, while an inductor is a catch all for nearly any component utilizing a coil of wire to create an electro-magnetic field. While, yes, a choke is an inductor, it is also a separate and distinct use for an inductor such as a transformer or generator in their respective and most basic form. <span style="font-size: smaller;" class="autosigned">—Preceding ] comment added by ] (]) 01:16, 29 July 2010 (UTC)</span><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->''

	DO NOT MERGE. The common mode choke is NOT an inductor. It is not use to store energy but to transform energy in heat. The unwanted common mode current is then dissipated. I will provide more datas in a couple of week on this topic. <span style="font-size: smaller;" class="autosigned">—Preceding ] comment added by ] (]) 08:02, 23 September 2010 (UTC)</span><!-- Template:UnsignedIP --> <!--Autosigned by SineBot-->

	== Parallels with Capacitor ==		== Parallels with Capacitor ==

	In the Capacitor article, they have a lovely section about Impedance and phaser voltage. Could we add one here too? I came here to find out <math> Z_L = \frac{V_L}{I_L} = 2 \pi j f L = j \omega L = j X_L </math> because I couldn't remember it for my homework, but it isn't here.		In the Capacitor article, they have a lovely section about Impedance and phaser voltage. Could we add one here too? I came here to find out <math> Z_L = \frac{V_L}{I_L} = 2 \pi j f L = j \omega L = j X_L </math> because I couldn't remember it for my homework, but it isn't here. <small class="autosigned">— Preceding ] comment added by ] (]) 23:13, 14 October 2008‎ (UTC)</small><!-- Template:Unsigned IP -->

	== Inductance formulae ==

	It would be super if someone adds figures next to each formula group so that people can see where are the variants (r,d etc.) exactly.--] (]) 09:18, 10 December 2008 (UTC)

	== wirewound resistors ==

	Everything has some inductance. All resistors are non-ideal and have inductance. How could one test a resistor to see if it is ordinary wirewound, with some inductance, or special-wirewound with low inductance, or some other non-inductive type? What is typical inductance of various types of resistors? How much inductance is likely to be "significant" for various purposes? Does the inductance of a wirewound resistor tend to be more significant in low-ohms or hi-ohms resistors?
	-] (]) 23:44, 1 July 2009 (UTC)

			== Purpose of an inductor? ==
	Extended discussion of the inductance of wirewound resistors, and how to measure it:
	* www.diyaudio.com/forums/showthread.php?s=&threadid=113209 * diyAudio Forums > Top >Loudspeakers >Loudspeakers >Resistor Inductance
	-] (]) 02:51, 3 July 2009 (UTC)
	: According to the discussion there, many wire-wound resistors have surprisingly high inductance (with values in mH); this is negligible for low frequency, but critical in radio applications. -- ] (]) 04:04, 4 May 2010 (UTC)

			Is the ''purpose'' of an inductor to slow or dampen the rate of change in a voltage or current? Or is its purpose something else?
	== Reactor? ==

			The article starts with "An inductor, also called a coil, choke, or reactor, is a passive two-terminal electrical component that stores energy in a magnetic field when electric current flows through it".
	Is there any evidence that "Reactor" is actually used to describe inductors? I have never heard the term, but maybe it's like "condenser" - not used at all in some places, used in others. (Hard to do a Google search because of those big nuky things that blow up when a tsunami hits them...) ] (]) 17:36, 13 April 2011 (UTC)

	~~:Yes,~~ ~~reactors~~ ~~are~~ ~~chokes.~~ ~~Google(inductor~~ ~~choke~~ ~~reactor)~~ and ~~you~~ ~~will~~ get ~~many~~ ~~hits~~ ~~sans~~ ~~nukes~~. ~~See~~ ~~also~~ ]. ] (]) 17:50, 13 ~~April~~ ~~2011~~ (UTC)		But there's no word on why that would be useful, and we quickly get into technical terms and equations. That's fine, but a statement of purpose would help. ] (]) 05:40, 21 June 2022 (UTC)
	:: In electric power transmission, it's usual to refer to "shunt reactors" meaning big air- or oil-insulated coils connected in parallel with loads, to regulate voltage; you also find "series reactors" usually used to limit short-circuit current. "Reactor" isn't used as much in the electronics industries. --] (]) 18:26, 13 April 2011 (UTC)

			:Yes, that’s its purpose. And I agree the lead sentence (and entire lead paragraph) is not very useful for general readers; it is more a description of how an inductor works than what it is ‘’for’’. The lead sentence might give the erroneous impression that inductors are energy storage devices. Readers have to go to the end of the introduction before they find out what it is used for.
	== Bad spot in the intro ==

			:Maybe the lead could be rewritten to include a brief description of what it does in a circuit.--]<sup><small>]</small></sup> 07:18, 21 June 2022 (UTC)
	The intro asserts that "Due to the time-varying magnetic field inside the coil, a voltage is induced." But that sentence leaves the innocent reader asking himself, "''What'' time-varying field? Who said anything about the field's varying over time? Why should it vary?"

			== Proximity effect ==
	I request that somebody who knows what he's talking about do something appropriate to fix that passage.—] (]) 03:00, 3 February 2012 (UTC)
	:See ] for the biggest mess since ], ] or even ]. Warning - contains adult themes and situations, not for the idealistic. --] (]) 18:00, 15 May 2012 (UTC)

			It two wires are adjacent to each other and carrying current in the opposite direction. Then the current density tends to concentrate beneath the adjacent surfaces. But in a coil the currents on adjacent wires are in the same direction.
	== the use of magnets ==

			Visualizing a tightly wound coil, a wire somewhere in the middle is being touched by six other wires carry current in the same direction. The result is that the current densities are pushed away from the points where the wires touch and towards the place where there are gaps. So, six regions of low density and six regions of high density as you go around the wire.
	The authors had failed to notice is that in one of the images (called coils.jpg) shows an inductor with a magnet on it. i have scrapped a 17inch computer monitor (branded "acer") and i found two of these (heatshrink over the top). what is the function of the magnet?
	] (]) 22:36, 5 March 2012 (UTC)

			I will take my shot at improving the text. ] (]) 22:37, 20 June 2024 (UTC)
	== Generalized Impedance ==

			:That's if the coil has multiple layers of tightly spaced windings in which the wires are parallel. Most high frequency coils either have single layer windings with the turns spaced apart, interleaved windings, or basket weave windings where the wires in succeeding layers are at angles to each other, to reduce proximity effect losses. They may also use litz wire. See the pictures in the article. --]<sup><small>]</small></sup> 04:12, 21 June 2024 (UTC)
	Why is there an equation only for impedance in the Laplace domain? Z = jωL is a pretty important equation, is it not? <span style="font-size: smaller;" class="autosigned">— Preceding ] comment added by ] (]) 17:57, 15 May 2012 (UTC)</span><!-- Template:Unsigned IP --> <!--Autosigned by SineBot-->
			::Yes. I'm just trying to get said in a sentence or two. ] (]) 05:16, 21 June 2024 (UTC)

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Induction loop

I suspect that the new Induction loop article needs to be merged with another (this one?); it certianly needs a lot of work by someone who knows what they're doing. Mel Etitis (Μελ Ετητης) 13:12, 30 Mar 2005 (UTC)

No kidding; Is there much in that article that's salvagable?

And shouldn't it be about the gadgets used to tap phones and detect cars at traffic signals?

Atlant 13:29, 30 Mar 2005 (UTC)

Deletion of old history section

I had hopped to save some bandwidth but if I must: First, it is wrong. Stanley didn’t invent the first practical induction coil as stated. Inductions coils had been around for fifty years before that and Ruhmkorff was building excellent ones in 1850. What Stanley’s patent did cover was a version of an AC transformer that proved to be practical and similar to modern transformers. Since patents require titles and there was not yet a word for the device, he used whatever words were handy. The patent was titled “Induction Coil”. Mr. Stanley’s contribution is covered in transformer where it belongs. It has nothing to do with the Inductor article. This history section was left over here as a remnant of some confusion in terminology from a year ago. Let us recreate a history section only when we have something applicable to put into it. Meggar 05:58, 2005 Jun 8 (UTC)

Thank you for that explanation.

Atlant 11:47, 8 Jun 2005 (UTC)

Parallels with Capacitor

In the Capacitor article, they have a lovely section about Impedance and phaser voltage. Could we add one here too? I came here to find out $Z_{L}={\frac {V_{L}}{I_{L}}}=2\pi jfL=j\omega L=jX_{L}$ because I couldn't remember it for my homework, but it isn't here. — Preceding unsigned comment added by 76.200.130.99 (talk) 23:13, 14 October 2008‎ (UTC)

Purpose of an inductor?

Is the purpose of an inductor to slow or dampen the rate of change in a voltage or current? Or is its purpose something else?

The article starts with "An inductor, also called a coil, choke, or reactor, is a passive two-terminal electrical component that stores energy in a magnetic field when electric current flows through it".

But there's no word on why that would be useful, and we quickly get into technical terms and equations. That's fine, but a statement of purpose would help. 73.127.147.187 (talk) 05:40, 21 June 2022 (UTC)

Yes, that’s its purpose. And I agree the lead sentence (and entire lead paragraph) is not very useful for general readers; it is more a description of how an inductor works than what it is ‘’for’’. The lead sentence might give the erroneous impression that inductors are energy storage devices. Readers have to go to the end of the introduction before they find out what it is used for.

Maybe the lead could be rewritten to include a brief description of what it does in a circuit.--Chetvorno 07:18, 21 June 2022 (UTC)

Proximity effect

It two wires are adjacent to each other and carrying current in the opposite direction. Then the current density tends to concentrate beneath the adjacent surfaces. But in a coil the currents on adjacent wires are in the same direction.

Visualizing a tightly wound coil, a wire somewhere in the middle is being touched by six other wires carry current in the same direction. The result is that the current densities are pushed away from the points where the wires touch and towards the place where there are gaps. So, six regions of low density and six regions of high density as you go around the wire.

I will take my shot at improving the text. Constant314 (talk) 22:37, 20 June 2024 (UTC)

That's if the coil has multiple layers of tightly spaced windings in which the wires are parallel. Most high frequency coils either have single layer windings with the turns spaced apart, interleaved windings, or basket weave windings where the wires in succeeding layers are at angles to each other, to reduce proximity effect losses. They may also use litz wire. See the pictures in the article. --Chetvorno 04:12, 21 June 2024 (UTC)

Yes. I'm just trying to get said in a sentence or two. Constant314 (talk) 05:16, 21 June 2024 (UTC)

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