- A charged particle moving perpendicular to a magnetic field experiences a Lorentz force \( F = qvB \), which provides the centripetal force for circular motion.
- Centripetal force required: \( F = \frac{m v^2}{r} \).
- Equate the forces:
\[
q v B = \frac{m v^2}{r}
\]
- Solve for \( r \):
\[
r = \frac{m v^2}{q v B} = \frac{m v}{q B}
\]
- This matches option (C).