T-I-1: Difference between revisions
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The Joukovski's transformation is defined by the following application | The Joukovski's transformation is defined by the following application | ||
<math> | <math> | ||
\begin{center} | |||
J: | J: | ||
\begin{array}[t]{ccc} | \begin{array}[t]{ccc} | ||
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z &\mapsto & z + \displaystyle \frac{1}{z} | z &\mapsto & z + \displaystyle \frac{1}{z} | ||
\end{array} | \end{array} | ||
\end{center} | |||
</math> | </math> |
Revision as of 15:32, 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 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, , the space of conformal mappings is much larger and one can show that, given an open set , any holomorphic function such that , defines a conformal map from to . 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
Failed to parse (unknown function "\begin{center}"): {\displaystyle \begin{center} J: \begin{array}[t]{ccc} \mathbb{C} \setminus \{ 0 \} &\to &\mathbb{C} \\ z &\mapsto & z + \displaystyle \frac{1}{z} \end{array} \end{center} }