Taylor–Maccoll flow
Flow behind a conical shock wave / From Wikipedia, the free encyclopedia
Taylor–Maccoll flow refers to the steady flow behind a conical shock wave that is attached to a solid cone. The flow is named after G. I. Taylor and J. W. Maccoll, whom described the flow in 1933, guided by an earlier work of Theodore von Kármán.[1][2][3]
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