A charged particle of mass \( m \) and charge \( q \) moves with a velocity \( \vec{v} \) perpendicular to a magnetic field \( \vec{B} \). The radius of the circular path it follows is:
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For a charged particle in a magnetic field, the radius of the circular path is derived by equating the magnetic force \( qvB \) to the centripetal force \( \frac{m v^2}{r} \).
- 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).
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