A charged particle is subject to a force in a magnetic field as described by the Lorentz force law:
\[
\vec{F} = q (\vec{v} \times \vec{B})
\]
where:
- \( \vec{F} \) represents the force exerted on the particle,
- \( q \) denotes the particle's charge,
- \( \vec{v} \) is the particle's velocity,
- \( \vec{B} \) signifies the magnetic field.
Based on this equation, a charged particle will experience no force under the following conditions:
1. Velocity parallel to the magnetic field:
When the particle's velocity is parallel or anti-parallel to the magnetic field (\( \vec{v} \parallel \vec{B} \) or \( \vec{v} = k \vec{B} \), where \( k \) is a scalar constant), the cross product \( \vec{v} \times \vec{B} \) becomes zero. Consequently, no force will be exerted on the particle.
2. Zero velocity:
If the charged particle is stationary (\( \vec{v} = 0 \)), no magnetic force will act upon it, as the force is contingent on the particle's velocity.
In summary, a charged particle experiences no force in a magnetic field when either:
- The particle is at rest, or
- The particle's velocity vector is aligned (parallel or anti-parallel) with the magnetic field vector.