(a) Electron angular momentum about the nucleus is an integer multiple of$\frac{h}{2\pi}$ , where $h$ is Planck’s constant.
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ I\omega\ = \ mvr$
= $\frac{nh}{2\pi}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ r \propto n$