Drag the conducting rod through the magnetic field. The free electrons feel a magnetic force F = qv × B and pile toward one end, leaving the other end positive — a motional EMF. Stop moving and they spread out evenly again.
A conductor holds a sea of free electrons. When the rod moves with velocity v through a
magnetic field B, each electron feels the magnetic force F = qv × B (with q = −e).
That force acts along the rod, sweeping electrons to one end so it becomes negative while the
far end is left positive. The separated charges set up an internal electric field that grows until it
balances the magnetic force — a steady motional EMF of size ε = BLv, where L is the
rod length. The build-up is proportional to speed and field strength, and reverses if you reverse either
the motion or the field. Stop moving (v = 0) and there is no magnetic force, so the electrons spread back
out evenly. Here the field points into or out of the screen and the rod is dragged in the screen plane,
so only motion perpendicular to the rod produces separation.