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Planar ionized gas (air) flow in the boundary layer under the conditions of the socalled equilibrium ionization is studied in this paper. The contour of the body within the fluid is porous. The ionized gas flows through the magnetic field of the power B m = B m (x)İt is assumed that the ionized gas electro-conductivity is a function of the ratio of the longitudinal velocity and the velocity at the outer edge of the boundary layer. Using the general similarity method, the governing boundarydoi:10.5937/spsunp1401011s fatcat:owsnfxbt55hixnvwuydcq5jyu4