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M_∞→1时圆球绕前体流场的数值模拟 被引量:1

Computation for Flow Field About a Sphere When M_∞→1
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摘要 本文根据来流马赫数M∞选取坐标变换函数,将M∞→1时的低超声速回球绕流前体流场变换到矩形的计算区域,忽略粘性影响,采用时间相关法,用TVD有限差分格式求Euler方程的定常解,得到了M∞=1.05、1.01和1.005的流场分布。 In this paper, a coordinate transformation was constructed according to Moo to convert the forward flow field about a sphere'into a rectangler area in the computational plane. Computation has been conducted for the inviscid flow field by solving Euler equations with time-dependent method and total variation diminishing(TVD) finite difference schemes. Flow field for M∞=1.05, 1. 01 and 1.005 have been obtained and locational of detached shock wave compare well with those obtained in ballistic facilities.
出处 《空气动力学学报》 CSCD 北大核心 1996年第1期104-109,共6页 Acta Aerodynamica Sinica
关键词 圆球 低超声速 TVD格式 欧拉方程 sphere low supersonic flow Euler equations TVDscheme
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参考文献2

  • 1郑之初,中国科学.A,1993年,23卷,7期,725页
  • 2郑之初,空气动力学学报,1984年,1卷,3期,98页

同被引文献16

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  • 5Klapproth J F. Approximate relative total pressure losses of an infinite cascade of supersonic blades with finile lead- ing-edge thickness[R]. NACA RM E9L21,1950.
  • 6Graham R C, Klapproth J F, Barina F J. Investigation of off-design performance of shock in rotor type supersonic blading[R]. NACA RM-E51C22,1951.
  • 7刘翠娥,吴文权.任意迥转面叶栅超声速进口流场特征线法计算机程序和唯一进气角的确定[J].工程热物理学报,1980,l(3):255-264.
  • 8吴仲华,吴文权,华耀南,等.给定激波模型的叶栅跨声流的计算[J].工程热物理学报,1984,5(3):256-261.
  • 9阮志坤.平面叶栅栅前激波的改进模型[J].工程热物理学报,1984,5(4):338-341.
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