The source of the force acting on a current-carrying conductor placed in a magnetic field is the magnetic interaction between the moving charges (current) in the conductor and the external magnetic field. The force on a current-carrying conductor in a magnetic field is given by:
\[
F = I L B \sin(\theta)
\]
Where:
- \( F \) is the force,
- \( I \) is the current,
- \( L \) is the length of the conductor in the magnetic field,
- \( B \) is the magnetic field strength,
- \( \theta \) is the angle between the magnetic field and the conductor.
For two long, straight, parallel conductors carrying steady currents \( I_1 \) and \( I_2 \), the force per unit length between them is given by Ampère's law:
\[
F = \frac{\mu_0 I_1 I_2}{2 \pi d}
\]
Where:
- \( \mu_0 \) is the permeability of free space,
- \( d \) is the distance between the two conductors.
This is the expression for the force between two parallel conductors carrying steady currents, and it defines Ampère's law.