2005
DOI: 10.1002/fld.916
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Shock wave numerical structure and the carbuncle phenomenon

Abstract: SUMMARYSince the development of shock-capturing methods, the carbuncle phenomenon has been reported to be a spurious solution produced by almost all currently available contact-preserving methods. The present analysis indicates that the onset of carbuncle phenomenon is actually strongly related to the shock wave numerical structure. A matrix-based stability analysis as well as Euler ÿnite volume computations are compared to illustrate the importance of the internal shock structure to trigger the carbuncle phen… Show more

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Cited by 108 publications
(49 citation statements)
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“…When applied to multi-dimensional flows, such one-dimensional approximations give rise to undesired numerical problems, especially for triangular or tetrahedral unstructured meshes [5]. For hypersonic applications, the carbuncle phenomenon takes place near the blunt nose region [6] and accurate computation of viscous flows with tetrahedral meshes remains a challenge [7]. Remedies for these numerical issues have been proposed and investigated but in general, lack robustness.…”
Section: Introductionmentioning
confidence: 99%
“…When applied to multi-dimensional flows, such one-dimensional approximations give rise to undesired numerical problems, especially for triangular or tetrahedral unstructured meshes [5]. For hypersonic applications, the carbuncle phenomenon takes place near the blunt nose region [6] and accurate computation of viscous flows with tetrahedral meshes remains a challenge [7]. Remedies for these numerical issues have been proposed and investigated but in general, lack robustness.…”
Section: Introductionmentioning
confidence: 99%
“…Remedies exist but in general, lack robustness. For hypersonic applications, carbuncle phenomenon takes place near the blunt nose region [2] and accurate computation of viscous flows with tetrahedral meshes remains a challenge [3].…”
Section: Introductionmentioning
confidence: 99%
“…Проблемы подобного плана обычно преодолеваются введением энтропийной коррекции [7] (ее введения оказывается недостаточно в случае достаточно силь-ных волн разрежения). Другие проблемы, возникающие при моделировании сверхзвукового обтекания затупленного тела, связаны с появлением грибовидного распределения плотности в окрестности точки торможения за фронтом головной ударной волны (carbuncle phenomenon) [8][9][10]. Методы, основанные на расщеплении вектора потока, не имеют указанной особенности.…”
Section: Introductionunclassified