Why is $\sqrt r \cos \frac \theta 2$ harmonic?
Why is $\sqrt r \cos \frac \theta 2$ harmonic?
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Keeping in mind that, in polar coordinates, the Laplacian looks like
$$\Delta = \frac {\partial^2} {\partial r^2} + \frac 1 r \frac \partial {\partial r} + \frac 1 {r^2} \frac {\partial^2} {\partial \theta^2}$$
and that "harmonic" means $\Delta f = 0$, it easy to check that in your case
$$\Delta f = - \frac 1 4 r^{-\frac 3 2} \cos \frac \theta 2 + \frac 1 r \left( \frac 1 2 r^{-\frac 1 2} \cos \frac \theta 2 \right) + \frac 1 {r^2} \left( -\frac 1 4 r^{\frac 1 2} \cos \frac \theta 2 \right) = 0 .$$
Unlike the approach based upon finding an analytic function such that $f$ should be its real or imaginary part, the approach based upon computing the Laplacian has the advantage of not depending on "inspiration", being purely computational (and thus algorithmic).
$$\sqrt{r}\cos \frac{\theta}{2}=Re(\sqrt{re^{i\theta}})=Re(\sqrt z)$$ The components of analytical functions are harmonic, so this is it.