A conductor of length \( l \) moving with velocity \( v \) perpendicular to a uniform magnetic field \( B \) induces an emf due to motional electromotive force.
Assume conductor along y-axis, magnetic field along z-axis, velocity along x-axis.
The induced emf is:
\[
e = B l v,
\]
derived from Lorentz force on charges: \( F = q (\vec{v} \times \vec{B}) \).
For perpendicular motion, the effective force separates charges, creating a potential difference \( e = B l v \).
Answer: \( e = B l v \).