Step 1: Understanding the Concept:
The particle moves in a circle in the plane perpendicular to the field. The magnetic force supplies the centripetal force: \(qvB=\dfrac{mv^2}{r}\), so \(mv=qBr\).
Step 2: Apply the Bohr quantisation:
Angular momentum: \(mvr=\dfrac{nh}{2\pi}\). Using \(mv=qBr\), we get \(qBr^2=\dfrac{nh}{2\pi}\), so \(r^2=\dfrac{nh}{2\pi qB}\).
Step 3: Find the energy:
All the energy is kinetic: \(E=\dfrac12mv^2=\dfrac12m\left(\dfrac{qBr}{m}\right)^2=\dfrac{q^2B^2r^2}{2m}\).
\[ E=\dfrac{q^2B^2}{2m}\cdot\dfrac{nh}{2\pi qB}=\dfrac{nhqB}{4\pi m} \]
Option D.
Step 4: Why the other options are wrong.
Options A, B and C are larger by factors of 8, 4 and 2. They come from dropping the factor \(\dfrac12\) in kinetic energy or the factor \(2\pi\) in the quantisation rule.
Final Answer:
The energy is n h q B / (4 pi m).
\[ \boxed{\text{(D) }\dfrac{nhqB}{4\pi m}} \]