Using Landau-Ginzburg-Devonshire theory we calculated numerically the static conductivity of charged domain walls with different incline angle with respect to spontaneous polarization vector in the uniaxial ferroelectrics-semiconductors of n-type. We used the effective mass approximation for the electron and holes density of states, which is valid at arbitrary distance from the domain wall.Due to the electrons accumulation, the static conductivity drastically increases at the inclined head-to-head wall by 1 order of magnitude for small incline angles θ~π/40 by up 3 orders of magnitude for the perpendicular domain wall (θ=π/2).There are space charge regions around the charged domain walls, but the quantitative characteristics of the regions (width and distribution of the carriers) appeared very different for the tail-to-tail and head-to-head walls in the considered donor doped ferroelectric semiconductor.The head-to-head wall is surrounded by the space charge layer with accumulated electrons and depleted donors of the same thickness (~40−100 correlation lengths). The tail-to-tail wall is surrounded by the thin space charge layer with accumulated holes of thickness ~5-10 correlation lengths and thick layer with accumulated donors of thickness ~100−200 correlation lengths, as well as the layer with depleted by electrons of thickness ~100−200 correlation lengths.* Corresponding author, e-mail: morozo@i.com.ua † Corresponding author, e-mail: vladimir.shur@usu.ru 2 The conductivity across the tail-to-tail wall is at least an order of magnitude smaller than the one of the head-to-head wall due to the low mobility of holes, which are improper carries.The results are in qualitative agreement with recent experimental data for LiNbO 3 doped with MgO.