Abstract
The transient energy transfer during expansion of a plane layer of radiating gas bounded by a strong shock is investigated. The inviscid, nonconducting gas is assumed to be perfect and in local thermodynamic equilibrium. A shock fitting procedure is used which completely specifies the motion and position of the shock by an iterative solution of the partial differential equations and the Rankine-Hugoniot shock boundary conditions. For a gray gas, results are presented for parameters of physical interest. Results obtained for transparent, gray, and nongray models are compared.
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