Conformal Mapping and flow normal to ellipse

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SUMMARY

The flow normal to an ellipse with a major axis of length 'a' and a minor axis of length 'b' is described by the equation φ = - (U b / E(e)) √(1 - (x²/a²) - (y²/b²)), where E(e) is the complete elliptical integral of the second kind and 'e' is the eccentricity. The discussion highlights the inadequacy of the Joukowski map for this transformation, suggesting instead the use of the mapping z → a cosh(ξ + i η) to achieve the desired functional form. The participant seeks clarity on how the complete elliptical integral influences the flow coefficient.

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  • Understanding of fluid dynamics, specifically flow around geometries.
  • Familiarity with conformal mapping techniques.
  • Knowledge of elliptical integrals, particularly the complete elliptical integral of the second kind.
  • Basic concepts of complex analysis and hyperbolic functions.
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  • Study the properties and applications of the complete elliptical integral of the second kind.
  • Explore advanced conformal mapping techniques relevant to fluid dynamics.
  • Investigate the Joukowski transformation and its limitations in different geometrical contexts.
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Mathematicians, fluid dynamicists, and engineers involved in the study of flow dynamics around elliptical shapes and those interested in advanced conformal mapping techniques.

nickthequick
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Hi,

Given that the flow normal to a thin disk or radius r is given by

\phi = -\frac{2rU}{\pi}\sqrt{1-\frac{x^2+y^2}{r^2}}

where U is the speed of the flow normal to the disk, find the flow normal to an ellipse of major axis a and minor axis b.

I can only find the answer in the literature in one place, where it's stated

\phi = -\frac{U b}{E(e)} \sqrt{1-\frac{x^2}{a^2}-\frac{y^2}{b^2}}

where E(e) is the complete elliptical integral of the second kind and e is the eccentricity of the disk.

I have been trying to use the Joukowski map to send lines of equipotential of the disk to those of the ellipse, but I'm not sure how the complete elliptical integral of the second kind enters this picture.

Any suggestions, references, would be appreciated!

Nick
 
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On second thought, the Joukowski map seems inappropriate here. I think the map I want is

z\to a \cosh(\xi + i \eta) so that
x=a\sinh (\xi) \cos(\eta) and y = a\cosh (\xi) \sin(\eta).

This will effectively give me the change in functional form that I expect; however, I still don't see how this will modify the coefficient in the appropriate way.
 

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