Step 1: Use Lorentz force for circular motion.
When a charged particle moves perpendicular to a magnetic field, it experiences a centripetal force due to magnetic force:
\[
F = qvB = \frac{mv^2}{r}
\]
Step 2: Solve for \( r \).
\[
qvB = \frac{mv^2}{r} \quad \Rightarrow \quad r = \frac{mv}{qB}
\]
So, the radius \( r \) is directly proportional to mass and velocity, and inversely proportional to charge and magnetic field.