But
it does help us to understand the basis of Faraday’s law when
the conductor is moving in a uniform and time-independent
magnetic field On the other hand, it is not obvious how an emf is induced when a
conductor is stationary and the magnetic field is changing – a fact which
Faraday verified by numerous experiments In the case of a stationary
conductor, the force on its charges is given by
F = q (E + v ´´´´´ B) = qE
(6 6)
since v = 0