Implicit LU-SGS algorithm for high-order methods on unstructured grid with p-multigrid strategy for solving the steady Navier-Stokes equations

被引:21
作者
Parsani, M. [1 ]
Van den Abeele, K. [1 ]
Lacor, C. [1 ]
Turkel, E. [2 ]
机构
[1] Vrije Univ Brussel, Dept Mech Engn, Fluid Dynam & Thermodynam Res Grp, B-1050 Brussels, Belgium
[2] Tel Aviv Univ, Dept Math, IL-69978 Tel Aviv, Ramat Aviv, Israel
关键词
Navier-Stokes; High-order methods; Implicit LU-SGS algorithm; Von Neumann analysis; p-Multigrid; FINITE VOLUME METHOD; DISCONTINUOUS GALERKIN METHOD; CONSERVATION-LAWS; ELEMENT-METHOD; EXTENSION; SCHEMES; STABILITY;
D O I
10.1016/j.jcp.2009.10.014
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
The fluid dynamic equations are discretized by a high-order spectral volume (SV) method on unstructured tetrahedral grids. We solve the steady state equations by advancing in time using a backward Euler (BE) scheme. To avoid the inversion of a large matrix we approximate BE by an implicit lower-upper symmetric Gauss-Seidel (LU-SGS) algorithm. The implicit method addresses the stiffness in the discrete Navier-Stokes equations associated with stretched meshes. The LU-SGS algorithm is then used as a smoother for a p-multigrid approach. A Von Neumann stability analysis is applied to the two-dimensional linear advection equation to determine its damping properties. The implicit LU-SGS scheme is used to solve the two-dimensional (2D) compressible laminar Navier-Stokes equations. We compute the solution of a laminar external flow over a cylinder and around an airfoil at low Mach number. We compare the convergence rates with explicit Runge-Kutta (E-RK) schemes employed as a smoother. The effects of the cell aspect ratio and the low Mach number on the convergence are investigated. With the p-multigrid method and the implicit smoother the computational time can be reduced by a factor of up to 5-10 compared with a well tuned E-RK scheme. (C) 2009 Elsevier Inc. All rights reserved.
引用
收藏
页码:828 / 850
页数:23
相关论文
共 35 条
[1]  
*AGARD, 1979, AR138 AGARD
[2]  
Barlow J.B., 1999, Low-speed wind tunnel testing
[3]  
BIJL H, 2001, 20012612 AIAA
[4]  
Brandt A., 1982, A Guide to Multigrid Development
[5]   Stability and convergence analysis of implicit upwind schemes [J].
Buelow, PEO ;
Venkateswaran, S ;
Merkle, CL .
COMPUTERS & FLUIDS, 2001, 30 (7-8) :961-988
[6]   The local discontinuous Galerkin method for time-dependent convection-diffusion systems [J].
Cockburn, B ;
Shu, CW .
SIAM JOURNAL ON NUMERICAL ANALYSIS, 1998, 35 (06) :2440-2463
[7]   The Runge-Kutta discontinuous Galerkin method for conservation laws V - Multidimensional systems [J].
Cockburn, B ;
Shu, CW .
JOURNAL OF COMPUTATIONAL PHYSICS, 1998, 141 (02) :199-224
[8]   TVB RUNGE-KUTTA LOCAL PROJECTION DISCONTINUOUS GALERKIN FINITE-ELEMENT METHOD FOR CONSERVATION-LAWS .2. GENERAL FRAMEWORK [J].
COCKBURN, B ;
SHU, CW .
MATHEMATICS OF COMPUTATION, 1989, 52 (186) :411-435
[9]   THE RUNGE-KUTTA LOCAL PROJECTION DISCONTINUOUS GALERKIN FINITE-ELEMENT METHOD FOR CONSERVATION-LAWS .4. THE MULTIDIMENSIONAL CASE [J].
COCKBURN, B ;
HOU, SC ;
SHU, CW .
MATHEMATICS OF COMPUTATION, 1990, 54 (190) :545-581
[10]   TVB RUNGE-KUTTA LOCAL PROJECTION DISCONTINUOUS GALERKIN FINITE-ELEMENT METHOD FOR CONSERVATION-LAWS .3. ONE-DIMENSIONAL SYSTEMS [J].
COCKBURN, B ;
LIN, SY ;
SHU, CW .
JOURNAL OF COMPUTATIONAL PHYSICS, 1989, 84 (01) :90-113