Resistance between two ferromagnetic electrodes coupled to a normal channel depends on their relative magnetizations. The spin-dependent component, R, of the resistance changes with magnetic field, B, normal to the directions of magnetizations. In the field of spin transport, this change, R(B), originating from the Larmour spin precession, is called the Hanle curve. We demonstrate that the shape of the Hanle curve evolves upon application of an ac drive and study this evolution theoretically as a function of the amplitude, B1, and frequency, ω, of the drive. If the distance between the electrodes, L, is smaller than the spin-diffusion length, λs, the prime effect of a weak circular-polarized drive is the shift of the center of the curve to the value of B for which the Larmour frequency, ωL, is ∼ B Linearly polarized drive has a fundamentally different effect on the Hanle curve, affecting not its shape, but rather its width.