The Joukowski map is a holomorphic function for , withA holomorphic function is a local conformal map wherever its derivative is nonzero. Hence the two finite nonzero critical points areThey lie on the boundary of the fluid region. At the displayed formula has a pole and is undefined as a map to the finite complex plane; zero is outside the fluid region. Thus is locally conformal everywhere in the fluid.
For ,Both factors are positive in the fluid region, so its image is contained in the upper half-plane. The boundary correspondence is also explicit: on the upper unit semicircle, gives , while the real rays and map onto the rays and .
To prove the image is the whole upper half-plane, fix any . The equation isIts roots have product one. Neither root can have unit modulus, since that would make real. Exactly one root therefore has modulus greater than one. For that root the formula for forces , so it belongs to the fluid region. Moreover, if , thenTwo distinct roots in the fluid region would require , impossible when both moduli exceed one. Thus the Joukowski map of the upper exterior of a unit disk is a bijection from the fluid region onto the upper half-plane.
The quadratic formula gives two algebraic possibilities. To select one consistent holomorphic square root, setwhere each factor is the principal square root. Both arguments lie in the upper half-plane, so neither crosses its branch cut. This choice satisfies and at large in the upper half-plane. The required inverse function isFor , , this gives , whose modulus exceeds one. As varies continuously in the upper half-plane, this root cannot cross , since that would make real. Hence the selected root always lies in the fluid region. The other root is its reciprocal and lies inside the unit disk. Simply writing the principal square root of would not specify this branch correctly throughout the upper half-plane.
Articles by others on the same topic
There are currently no matching articles.