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 Thus, any force on the charge must arise from the electric
field term E alone