Step 1: Understand the context of electromagnetic force on a charge
A charged particle moving in an electric and magnetic field experiences forces due to both fields.
These forces are fundamental interactions described by classical electromagnetism.
Step 2: Electrostatic force
The electric field \( \vec{E} \) exerts a force on a charge \( q \) given by:
\( \vec{F_1} = q \vec{E} \)
This is called the electrostatic force.
It acts in the direction of the electric field for a positive charge, and opposite for a negative charge.
Step 3: Magnetic force
When a charge \( q \) moves with velocity \( \vec{v} \) in a magnetic field \( \vec{B} \), it experiences a magnetic force given by the vector cross product:
\( \vec{F_2} = q(\vec{v} \times \vec{B}) \)
This force is perpendicular to both the velocity vector and the magnetic field, as per the right-hand rule.
It depends on the magnitude of \( v \), the strength of \( B \), and the sine of the angle between them.
Step 4: Combine both forces (Lorentz Force Law)
The total electromagnetic force \( \vec{F} \) acting on a moving charge in electric and magnetic fields is given by:
\( \vec{F} = \vec{F_1} + \vec{F_2} = q\vec{E} + q(\vec{v} \times \vec{B}) \)
Final Answer:
\( \vec{F_1} = q \vec{E}, \vec{F_2} = q(\vec{v} \times \vec{B}) \)