期刊文献+

积分梯度法的两种格式 被引量:2

Two Schemes of Integrated Gradient Method
下载PDF
导出
摘要 在二维柱坐标系下Lagrange流体力学的计算中,积分梯度法是动量方程的一种有效离散方法.积分梯度法中,IGT(Integral Gradient Total)格式不能保持柱几何下一维球对称性;IGA(Integral Gradient Average)格式可以保持一维球对称性,但当相邻网格质量相差比较大时,会得到远远脱离真实物理现象的加速度.深入研究IGA和IGT格式发现,当相邻网格边界压力取为质量加权时,即使相邻网格质量相差较大,对于一维平面和一维柱问题,IGT与IGA等价;在二维情形下,可以缩小IGT和IGA之间的差异.理论证明,IGA格式不能保持系统的动量守恒,IGT格式能保持系统的动量守恒性.数值模拟结果进一步显示了这两个格式的优缺点. In a cylinderical coordinate system, integrated gradient method is an effective discrctization for equations of Lagrangian hydrodynamics. In the method IGT (Integral Gradient Total) scheme does not preserve spherical symmetry while IGA (Integral Gradient Average) scheme overcomes nonsymmetry in cylinderical coordinate system. However, IGA results in abnormally large acceleration in case of large mass ratios, where the mass of one subcell around a node is smaller than that of the other three subcells. If boundary force between neighbouring cells is taken as weighted mass average, IGA scheme is equivalent to IGT scheme in both a planar problem and a cylinderical problem even if there exists a large mass ratio. It is shown that IGT scheme preserves total momentum conservation but IGA scheme does not. Numerical results demonstrate advantages and disadvantages of the two schemes.
出处 《计算物理》 EI CSCD 北大核心 2008年第5期525-534,共10页 Chinese Journal of Computational Physics
基金 国家863高技术惯性约束聚变主题、中物院科学技术发展基金(2007B09009,2007A09002) 中物院科学技术基金(20060106) 计算物理国家重点实验室项目(9140C6902010603) 国家自然科学基金(10572028)资助项目
关键词 积分梯度法 IGT格式 IGA格式 球对称性 守恒性 integrated gradient method integral gradient total scheme integral gradient average scheme spherical symmetry conservation
  • 相关文献

参考文献3

二级参考文献8

共引文献15

同被引文献15

  • 1勇珩,段庆生,裴文兵,江松.二维三温能量方程的差分格式及平面靶数值模拟[J].计算物理,2005,22(6):479-487. 被引量:6
  • 2勇珩,袁国兴,裴文兵,古培俊.空腔靶大变形问题的网格构造[J].计算物理,2007,24(1):1-6. 被引量:3
  • 3Lindl J.Development of the indirect-drive approach to inertial confinement fusion and the target physics basis for ignition and gain[J].Phys Plasmas,1995,2(11):3933-4023.
  • 4Paisner J A,Campbell E M,Hogan W J.The National Ignition Facility project[J].Fusion Technol,1994,26:755-766.
  • 5Holstein P A,Chaland F,Charpin C,et al.Evolution of the target design for the MJ laser[J].Laser Part Beams,1999,17:403-413.
  • 6Benson D J.Computational methods in Lagrangian and Eulerian hydrocodes[J].Comput Meth Appl Mech Eng,1992,99:235-394.
  • 7Hirt C W,Amsden A A,Cook J L.An arbitrary Lagrangian-Eulerian computing method for all flow speeds[J].J Comput Phys,1974,14:227-253.
  • 8Barton R T.Development of a multi-material two-dimensional,arbitrary Lagrangian-Eulerian mesh computer program,in numerical astrophysics[M].Boston:Jones and Bartlett Publishers,1985:482-497.
  • 9Harte J A,Alley W E,Bailey D S,et al.LASNEX-A 2-D physics code for modeling ICF[R].UCRL-LR-105821-96-4,1996:150-164.
  • 10Marinak M M,Kerbel G D,Gentile N A,et al.3D HYDRA simulations of NIF targets[R].UCRL-JC-141084-REV-1,2000.

引证文献2

二级引证文献5

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部