Abstract
The pattern of diffraction at the gas-liquid interface, induced by a system of oncoming shock waves of regular interaction in gas impinging on a wedge submerged in the liquid is considered. The wedge of arbitrary angle has its apex at the unperturbed interface with one of its sides at a nearly straight angle to the liquid unperturbed surface. The liquid is assumed only slightly compressible, which makes it possible to consider the problem in linear formulation by the method proposed in /1–3/.
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