Two dimensional fluid flow is naturally modelled by complex functions, which operate on complex numbers (each complex number has real and imaginary components, so is two dimensional) and return complex numbers, which are the components of the velocity in the real and imaginary directions.
If we assume that
-
The fluid flow is continuous and the fluid velocity is continuous
-
The fluid flow is two dimensional
-
The fluid flow is steady
then we can represent the velocity of the fluid at each point by a continuous complex function
whose domain is the region occupied by the fluid.
In fact we must have
with
and![]()
To find the flow in a direction at angle
anticlockwise from the real axis (
since anticlockwise is taken to be in the positive sense) relative to the real axis we can rotate
by the angle
then take the real part, so that
where
is the complex conjugate of
and similarly![]()
We are interested in the real part of
and this is the same if we take the complex conjugate of
The conjugate of
is in some ways more useful than![]()
Theorem
A steady two dimensional fluid flow with continuous velocity function
on a region
is a model flow ( circulation and flux free, so that the fluid has constant density) if and only the conjugate velocity function bar v is analytic on![]()
Any function
analytic on a region
can be considered as the conjugate velocity function of a continuous velocity function
on![]()
Example: If
(
is analytic on
then
is the model flow velocity function.