In spherical coordinates, we have \begin{align} x&=r\sin\theta\cos\phi\\ y&=r\sin\theta\sin\phi\\ z&=\cos\theta \end{align} If we look at \(\theta=\frac{\pi}{2}\), then \(\sin\theta=1\) and \(\cos\theta=0\). With these restrictions, we have: \begin{align} x&=r\cos\phi\\ y&=r\sin\phi\\ z&=0 \end{align} These are plane polar coordinates.
(Quick) Purpose: Recall the relationship between conservative forces and potentials.
Show that a central force is always conservative. Find the scalar potential \(U\) corresponding to the central force \(\vec{F}=f(r)\,\hat{r}\) and show that it depends only on the distance from the center of mass, i.e. \(U=U(r)\).