A charged particle experiences a force in a magnetic field according to the Lorentz force law:
\[
\vec{F} = q (\vec{v} \times \vec{B})
\]
where:
- \( \vec{F} \) is the force on the particle,
- \( q \) is the charge of the particle,
- \( \vec{v} \) is the velocity of the particle,
- \( \vec{B} \) is the magnetic field.
From this equation, we can conclude that the charged particle will not experience a force in the following cases:
1. When the velocity of the particle is parallel to the magnetic field:
If the velocity of the charged particle is parallel or anti-parallel to the magnetic field (\( \vec{v} \parallel \vec{B} \) or \( \vec{v} = k \vec{B} \) where \( k \) is a constant), then the cross product \( \vec{v} \times \vec{B} \) will be zero, and therefore, the particle will not experience any force.
2. When the velocity of the particle is zero:
If the charged particle is at rest (\( \vec{v} = 0 \)), then no force will act on it, as the magnetic force depends on the velocity of the particle.
Thus, a charged particle does not experience a force in a magnetic field if:
- The particle is at rest, or
- The particle’s velocity is parallel (or anti-parallel) to the magnetic field.