Abstract
Sound pulses in which the disturbed region has small or large optical thickness are considered. An analogy is drawn between the influence on the non-stationary velocity field structure of radiant energy transport and of chemical transformations occurring in reacting mixtures. This analogy embraces both completely dispersed shock waves, and waves including discontinuities with incomplete dispersion. The present paper continues the section and figure numbering used in part I [1]. Our aim is to apply the approximate equations derived in [I] to the study of the structure of weak shock waves in a radiating gas.
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