Misplaced Pages

Compressible flow: Difference between revisions

Article snapshot taken from Wikipedia with creative commons attribution-sharealike license. Give it a read and then ask your questions in the chat. We can research this topic together.
Browse history interactively← Previous editNext edit →Content deleted Content addedVisualWikitext
Revision as of 12:47, 28 June 2006 edit128.173.190.56 (talk) External links← Previous edit Revision as of 01:49, 10 July 2006 edit undo209.32.159.25 (talk)No edit summaryNext edit →
Line 29: Line 29:
stream tube in an accelerating flow contracts. But in a supersonic stream tube in an accelerating flow contracts. But in a supersonic
flow, a stream tube in an accelerating flow expands. To interpret this flow, a stream tube in an accelerating flow expands. To interpret this
in another way, consider steady flow in a tube that has a sudden expansion: in another way, c <sup></sup>onsider steady flow in a tube that has a sudden expansion:
the tube's cross section suddenly widens, so the cross-sectional area the tube's cross section suddenly widens, so the cross-sectional area
increases. increases.
Line 38: Line 38:
supersonic flow allows the density to change, the volume flux is not supersonic flow allows the density to change, the volume flux is not
constant. constant.

]
==External links==
*

Revision as of 01:49, 10 July 2006


A compressible flow is a situation in which the density of the flow cannot be assumed to be constant. In general, this is the case where the Mach number in part or all of the flow approaches or exceeds 0.3 (This is rather arbitrary but is a rule of thumb generally used). It can be proved that for flows with mach number less than 0.3 the change in density is less than 5%.

For subsonic compressible flows, it is sometimes possible to model the flow by applying a correction factor to the answers derived from incompressible calculations or modelling - for example, the Glauert-Prandtl rule

a c a i 1 1 M 2 {\displaystyle {\frac {a_{c}}{a_{i}}}\sim {\frac {1}{\sqrt {1-M^{2}}}}}

(ac is compressible lift curve slope, ai is the incompressible lift curve slope, and M is the Mach number).

For many other flows, their nature is qualitatively different to subsonic flows. A flow where the local Mach number reaches or exceeds 1 will usually contain shock waves. A shock is an abrupt change in the velocity, pressure and temperature in a flow; the thickness of a shock scales with the molecular mean free path in the fluid (typically a few micrometers).

Shocks form because information about conditions downstream of a point of sonic or supersonic flow can not propagate back upstream past the sonic point.

The behaviour of a fluid changes radically as it starts to move above the speed of sound (in that fluid). For example, in subsonic flow, a stream tube in an accelerating flow contracts. But in a supersonic flow, a stream tube in an accelerating flow expands. To interpret this in another way, c onsider steady flow in a tube that has a sudden expansion: the tube's cross section suddenly widens, so the cross-sectional area increases.

In subsonic flow, the fluid speed drops after the expansion (as expected). In supersonic flow, the fluid speed increases. This sounds like a contradiction, but it isn't: the mass flux is conserved but because supersonic flow allows the density to change, the volume flux is not constant.

Category: