1976
DOI: 10.1017/s0022112076003182
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Precursor shock waves at a slow—fast gas interface

Abstract: This paper presents experimental data obtained for the refraction of a plane shock wave at a carbon dioxide–helium interface. The gases were separated initially by a delicate polymer membrane. Both regular and irregular wave systems were studied, and a feature of the latter system was the appearance of bound and free precursor shocks. Agreement between theory and experiment is good for regular systems, but for irregular ones it is sometimes necessary to take into account the effect of the membrane inertia to o… Show more

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Cited by 62 publications
(27 citation statements)
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“…Their results indicate that on the beryllium side of the explosive, a compression wave in the beryllium drives a shock in the explosive ahead of the detonation wave. This is somewhat akin to what happens at fast-slow interfaces in gases [9]. However, in our subsonic inert flow case, we do not expect a shock in the confiner when steady state is achieved.…”
Section: Free Outer Boundary Problemsupporting
confidence: 64%
“…Their results indicate that on the beryllium side of the explosive, a compression wave in the beryllium drives a shock in the explosive ahead of the detonation wave. This is somewhat akin to what happens at fast-slow interfaces in gases [9]. However, in our subsonic inert flow case, we do not expect a shock in the confiner when steady state is achieved.…”
Section: Free Outer Boundary Problemsupporting
confidence: 64%
“…Their results are in excellent and Glaz [14], and Colella and Woodward [17] for the agreement with the shock refraction experiments of compressible Euler equations for a single material. This Abd-el-Fattah and Henderson [1][2][3] and Jahn [24]. methodology is second-order accurate in regions of smooth…”
Section: Introductionmentioning
confidence: 98%
“…The material properties and {i will determine which one is present as a~ increases towards transition to an irregular system. By definition, regular refraction ends at the shock critical angle ai = ctsc (43) Both experiments (Abdel-Fattah et al 1976;Abdel-Fattah and Henderson 1978b) and numerical results (Henderson et al 1990a(Henderson et al , 1990b show that the criterion which determines this condition is at, or close to, the point where there is sonic flow downstream of the t shock. For ct, i > o~8c, the A~ -1 matrix has unreal elements so the yon Neumann theory provides no physically realistic solutions.…”
Section: Slow-fast Refraction N <mentioning
confidence: 94%