The magnetic moment (µ) of a revolving electron around the nucleus varies with principal quantum number n as |
$\mu \propto n$ $\mu \propto 1 / n$ $\mu \propto n^2$ $\mu \propto 1 / n^2$ |
$\mu \propto n$ |
$\mu = IA = \frac{Q}{T} A \propto n$ Since $ A = \pi r^2 \propto n^4$ $ T \propto n^3$ |