The Cauchy – Riemann equations lay down the conditions for a complex valued function to be differentiable at a point, but they also have applications in fluid dynamics. If then
is differentiable at a point if:
Let the functionsand
be the horizontal and vertical components of the velocity field of a steady incompressible, irrotational flow in two dimensions. The equations are occur in fluid mechanics from consideration of the velocity potential
and
are found from the velocity potential
The condition that the flow be incompressible is that
and the condition that the flow be irrotational is that
- If we define the differential of a function
by
then the incompressibility condition is the integrability condition for this differential: the resulting function is actually the stream function because it is constant along flow lines. The first derivatives of
are given by
and the irrotationality condition implies that
satisfies the Laplace equation:
The harmonic function
(harmonic since
) that is conjugate to
is the velocity potential.
Every analytic function corresponds to a steady incompressible, irrotational fluid flow in the plane. The real part is the velocity potential, and the imaginary part is the stream function.