The spin density wave (SDW) in organic conductors like (TMTSF) 2PF 6 possesses two distinct collective modes; the spin wave and the sliding mode. Since the spin dynamics of SDW is described by an equation similar to the Leggett equation for superfluid 3He, we predict the longitudinal resonance. On the other hand both the electric charge and the current couple to the sliding SDW mode, which gives rise to a variety of nonlinear phenomena similar to those found in the quasi-one dimensional charge density wave (CDW) like NbSe 3.