Abstract

In the theortical investigation of heat and mass transfer in a nuclear reactor there has recently been steadily increasing use of the porous-body model [i-3]. The efficiency of this approach is especially apparent in calculating the fields of the heat-carrier velocity and temperature in geometrically complex objects consisting of several elements differing in their hydraulic and thermophysical properties. The motion of a viscous incompressible liquid in an anisotropic porous body is described by the continuity equation

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