FLOW INTO A BLACK HOLE
A simple model is proposed to describe the flow into a black hole from the turbulent flow of matter in initially circular orbits about the black hole. Magnetic effects are not considered. The shear between fluid elements at slightly different orbital radii causes turbulent eddies to be formed. These eddies determine the dissipation rate of kinetic energy into thermal energy. For approximately circular orbits, the magnitude of the gravitational potential energy is always equal to twice the kinetic energy; the destruction of the latter resulting in a reduction in the orbital radius and hence the potential energy. In this model, the turbulent eddy rotation period is presumed to be determined by the gradient in the gravity acceleration, leading to an eddy period proportional to the orbital period. If the flow speeds are supersonic but not relativistic, then the turbulent eddy size is set by the product of the eddy rotation period and the speed of sound. At a certain smaller radius, the orbital speeds and hence the dissipation rate are so great that the speeds become relativistic and the molecular speed tends toward its limit [Formula: see text]. Then the effective eddy size is controlled by the product of the eddy rotation period and the speed of light. Using these estimates for the important eddy size, the dissipation rate, temperature, density and sinking speed as a function of the orbital radius and the rate of mass flow into the black hole are derived. Subject headings: accretion, accretion disks, stars evolution, turbulence, eddy, sonic eddy.