Magnetic fields exert a force on moving electric charges, which is known as the Lorentz force. The force on a charged particle due to a magnetic field is given by the equation:
\[
\vec{F} = q (\vec{v} \times \vec{B})
\]
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 fiel(D)
For a charge that is at rest, the velocity \( \vec{v} = 0 \), which means the cross product \( \vec{v} \times \vec{B} = 0 \). Therefore, there is no force acting on a stationary electric charge when it is placed in a magnetic fiel(D)
However, for a moving charge, a current-carrying conductor, or a moving permanent magnet, the magnetic field exerts a force. Thus, the correct option is that a magnetic field does not interact with an electric charge at rest.