Step 1: Understanding the Concept
A charge moving perpendicular to a magnetic field follows a circle. The magnetic force supplies the centripetal force: \(qvB = \dfrac{mv^2}{r}\), so \(r = \dfrac{mv}{qB}\).
Step 2: Period
\[ T = \frac{2\pi r}{v} = \frac{2\pi m}{qB} \]
The period depends on the mass, the charge and the field, but the speed v cancels out. So the period is independent of the velocity of the particle, option (B).
Final Answer:
The period is independent of the velocity, option (B).
\[ \boxed{T = \frac{2\pi m}{qB}} \]