The electrical resistivity of nickel alloys. if extrapolated to B = 0. depends on the angle between the current and the magnetization. We have measured. at 4.2 K. this resistivity anisotropy for ternar) alloys of general composition Ni,,A, -xBx, where A and B denote different metallic elements. These alloys include Ni(A1Cr). Ni(AuCo). Ni(AuRh). Ni(CoRh). Ni(CoRu). Ni(CrFe). Ni(CrMn). Ni(CrSn). Ni(CrTi), Ni(CuRh), Ni(CuRu). Ni(CuV). Ni(FePt). Ni(FeRe), Ni(RhRu) and Ni(RuTi).The experimental results have been analysed in terms of Mott's two current conduction model. In this model it is assumed that the conduction electrons of spin direction parallel or antiparallel to the magnetization contribute individually to the current. Each impurity element in nickel has got two residual resistivities, one for each spin current. We have derived thest residual resistivities for the ferromagnetic moment parallel and perpendicular to the current. It is found that the resistivity anisotropy is large for one of the spin currents (about + IOo,) while that for the other varies around -20".