Step 1: Understanding the Concept:
In Bohr's model, the total energy in the \(n\)th orbit is \(E=-\dfrac{13.6}{n^2}\) eV, so its magnitude is \(|E|\propto\dfrac1{n^2}\). The angular momentum is \(L=\dfrac{nh}{2\pi}\), so \(L\propto n\).
Step 2: Combine:
Since \(n\propto L\), we get
\[ E\propto\frac1{n^2}\propto\frac1{L^2}=L^{-2} \]
Step 3: Choose:
Option (C).
Final Answer:
E is proportional to L to the power -2.
\[ \boxed{E\propto L^{-2}} \]