In short, then
(1) a conductor begins to move in the magnetic field
. It is clear. But when then ,
and then . That is .
(2) a conductor outside homogeneous magnetic field. In this case based on classic ideas I got (for wire 1 mm x 1 mm)
where
q - the charge of electron;
n - the concentration of electrons in the conductor;
x - thickness of the conductor (I assumed that the conductor was rectangular and made of copper).