Using the concept of induced electromotive force (emf) in a moving conductor within a magnetic field, we have the following relations:
- The induced emf \( \mathcal{E} \) in the rod is given by:
\[
\mathcal{E} = B \cdot v \cdot l
\]
- The magnetic force on the rod is given by:
\[
F = q \cdot \mathcal{E} = q \cdot B \cdot v \cdot l
\]
- From Newton’s second law, the force is also:
\[
F = m \cdot a
\]
Equating the two expressions for force:
\[
m \cdot a = q \cdot B \cdot v \cdot l
\]
Thus, solving for \( q \):
\[
q = \frac{m \cdot v}{B \cdot l}
\]