If [itex]f(z)=u(x,y)+iv(x,y)[/itex] is analytic in some region of the [itex]z[/itex] plane, then at every point in the region the Cauchy-Riemann conditions are satisfied:
[tex]\frac{ \partial u }{ \partial x } = \frac{ \partial v }{ \partial y } \quad \text{and} \quad \frac{ \partial u }{ \partial y } = -\frac{ \partial v }{ \partial x }[/tex]
and therefor:
[tex]\frac{ \partial^2 u }{ \partial x^2 } = \frac{ \partial^2 v }{ \partial x \partial y } \quad \text{and} \quad \frac{ \partial^2 u }{ \partial y^2 } = -\frac{ \partial^2 v }{ \partial y \partial x }[/tex]
provided these second derivatives exist. In fact,one can show that if [itex]f(z)[/itex] is analytic in some region [itex]R[/itex], all its derivative exist and are continuous in [itex]R[/itex]. Equating the two cross terms, we obtain
[tex]\frac{ \partial^2 u }{ \partial x^2 } + \frac{ \partial^2 u }{ \partial y^2 } = 0[/tex]
throughout the region [itex]R[/itex].
Similarly, by differentiating the first of the Cauchy-Riemann equations with respect to [itex]y[/itex], the second with respect to [itex]x[/itex], and subtracting we obtain
[tex]\frac{ \partial^2 v }{ \partial x^2 } + \frac{ \partial^2 v }{ \partial y^2 } = 0[/tex]
Equations (6.12a) and (6.12b) are Laplace's partial differential equations in two independent variables [itex]x[/itex] and [itex]y[/itex]. Any function that has continuous partial derivatives of second order and that satisfies Laplace's equation is called a harmonic function.
We have shown that if [itex]f(z)=u(x,y)+iv(x,y)[/itex] is analytic, then both [itex]u[/itex] and [itex]v[/itex] are harmonic functions. They are called conjugate harmonic functions.