Next: Cauchy-Riemann Relations
Up: Two-Dimensional Potential Flow
Previous: Introduction
The complex variable is conventionally written
![$\displaystyle z = x + {\rm i}\,y,$](img1933.png) |
(6.1) |
where
represents the square root of minus one. Here,
and
are both real, and are identified with the corresponding
Cartesian coordinates.
(Incidentally,
should not be confused with a
-coordinate: this is a strictly two-dimensional discussion.)
We can also write
![$\displaystyle z = r\,{\rm e}^{\,{\rm i}\,\theta},$](img1935.png) |
(6.2) |
where
and
are the modulus and
argument of
, respectively, but can also be identified with the corresponding plane polar coordinates.
Finally, Euler's theorem (Riley 1974),
![$\displaystyle {\rm e}^{\,{\rm i}\,\theta}= \cos\theta+{\rm i}\,\sin\theta,$](img1938.png) |
(6.3) |
implies that
We can define functions of the complex variable,
, in the same way that we
define functions of a real variable. For instance,
For a given function,
, we can substitute
and write
![$\displaystyle F(z) = \phi(x, y) + {\rm i}\,\psi(x, y),$](img1948.png) |
(6.8) |
where
and
are real two-dimensional functions. Thus, if
![$\displaystyle F(z) = z^{\,2},$](img1951.png) |
(6.9) |
then
![$\displaystyle F(x + {\rm i}\,y) = (x+{\rm i}\,y)^2 = (x^{\,2}-y^{\,2}) + 2\,{\rm i}\, x\,y,$](img1952.png) |
(6.10) |
giving
Next: Cauchy-Riemann Relations
Up: Two-Dimensional Potential Flow
Previous: Introduction
Richard Fitzpatrick
2016-01-22