1982
DOI: 10.1007/bf01089717
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Three-dimensional shape of a body of minimum drag in a hypersonic gas stream

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Cited by 2 publications
(1 citation statement)
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“…This differs from the standard bullet TD formed by a moving source, which is typically regular and convex. The observed TD geometry is rather unexpected to form naturally in a steady flow, as convex regions typically generate additional shocks (e.g., Grishin & Pogorelov 1988;Chen & Feldman 2015, and references therein), instabilities (e.g., Morton 1996;Panaras & Drikakis 2011, and references therein), and drag (except in special cases; e.g., Gusarov & Levin 1982;Plakhov 2016). The evolving flow around the TD is not expected to be steady, especially not so close to nearest passage, but as we show below, gasdynamic effects including instabilities do not naturally explain the observed bullet morphology.…”
Section: Bullet Cluster: Protruding Headmentioning
confidence: 99%
“…This differs from the standard bullet TD formed by a moving source, which is typically regular and convex. The observed TD geometry is rather unexpected to form naturally in a steady flow, as convex regions typically generate additional shocks (e.g., Grishin & Pogorelov 1988;Chen & Feldman 2015, and references therein), instabilities (e.g., Morton 1996;Panaras & Drikakis 2011, and references therein), and drag (except in special cases; e.g., Gusarov & Levin 1982;Plakhov 2016). The evolving flow around the TD is not expected to be steady, especially not so close to nearest passage, but as we show below, gasdynamic effects including instabilities do not naturally explain the observed bullet morphology.…”
Section: Bullet Cluster: Protruding Headmentioning
confidence: 99%