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* Study the conformal map <math>J</math> in the vicinity of <math> z = 1</math>: we consider a "smooth" curve <math>\gamma</math> passing through <math>z=1</math>, with a well defined tangent. Show that the image of <math>\gamma</math> exhibits a cusp in <math>J(1)</math>. In this purpose, we parametrize this curve <math>\gamma</math> by <math>z(t) </math> with <math>z(0)=1</math> and  <math>z'(0) \neq 0</math>. Write then the Taylor expansion of <math>z<\math> in <math>t=0</math> up to first order and the expansion of <math>J</math> close to <math>1</math> up to second order.
* Study the conformal map <math>J</math> in the vicinity of <math> z = 1</math>: we consider a "smooth" curve <math>\gamma</math> passing through <math>z=1</math>, with a well defined tangent. Show that the image of <math>\gamma</math> exhibits a cusp in <math>J(1)</math>. In this purpose, we parametrize this curve <math>\gamma</math> by <math>z(t) </math> with <math>z(0)=1</math> and  <math>z'(0) \neq 0</math>. Write then the Taylor expansion of <math>z</math> in <math>t=0</math> up to first order and the expansion of <math>J</math> close to <math>1</math> up to second order.

Revision as of 16:32, 14 October 2011


Analytical functions: conformal map and applications to hydrodynamics

This homework deals with the application of conformal maps to the study of two-dimensional hydrodynamics. A conformal map is a geometrical transformation which preserves all (oriented) crossing angles between lines. In dimension d3 a conformal map is necessarily composed from the following limited number of transformations: translations, rotations, homothetic transformation and special conformal transformation (which is the composition of a reflection and an inversion in a sphere). However in two dimensions, d=2, the space of conformal mappings is much larger and one can show that, given an open set Ω, any holomorphic function f:Ω such that $f(z)0$, zΩ defines a conformal map from Ω to f(Ω). The aim of this HW is to exploit this property to study some hydrodynamic flows in two spatial dimensions.


Joukovski's transformation

The Joukovski's transformation is defined by the following application

J:{0}zz+1z
  • Compute J(z) and deduce from it the maximal ensemble on which J is a conformal map. Show that J is always surjective. Under which condition on the set Ω the application J on Ω is surjective ? Give some examples of such (maximal) ensembles.
  • Give the image by J of the following sub-sets: (a) the half-line passing through the origin O and making an angle α with the x-axis, (b) the circle centered at the origin of radius R (analyse in particular the case R=1). What is the image, by J, of the outside of the unit circle |z|>1.

Hint: it might be useful to use polar coordinates, writing z=reiθ.


  • Get a better idea of this Joukowski's transformation using the following code in Mathematica:


Jouk[z_] := z + 1/z Jouk[1 - R Sin[\[Alpha]] + R Cos[u] + I (R Cos[\[Alpha]] + R Sin[u])]; ParametricPlot[{Re[%], Im[%]} /. {R -> 1.15, \[Alpha] -> 1.3}, {u, 0, 2 \[Pi]}, PlotRange -> {{-3, 3}, {-1, 1}}, AspectRatio -> 1/3]


  • Study the conformal map J in the vicinity of z=1: we consider a "smooth" curve γ passing through z=1, with a well defined tangent. Show that the image of γ exhibits a cusp in J(1). In this purpose, we parametrize this curve γ by z(t) with z(0)=1 and z(0)0. Write then the Taylor expansion of z in t=0 up to first order and the expansion of J close to 1 up to second order.