Global spectral analysis of multi-level time integration schemes: Numerical properties for error analysis

被引:10
作者
Sengupta, Tapan K. [1 ]
Sengupta, Aditi [2 ]
Saurabh, Kumar [1 ]
机构
[1] IIT Kanpur, Dept Aerosp Engn, High Performance Comp Lab, Kanpur 208016, Uttar Pradesh, India
[2] Univ Cambridge, Dept Engn, Cambridge CB2 1TN, England
关键词
Three-time level integration method; Global spectral analysis; Spurious mode; Adams-Bashforth method; Absolute instability; Effects of filtering; NAVIER-STOKES EQUATIONS; FINITE-DIFFERENCE SCHEMES; VELOCITY-VORTICITY FORMULATION; RAYLEIGH-TAYLOR INSTABILITY; TURBULENT HEAT-TRANSFER; CHANNEL FLOW; WAVE-PROPAGATION; REYNOLDS; DNS; SIMULATION;
D O I
10.1016/j.amc.2017.01.026
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
An analysis is reported here for three-time level integration methods following the global spectral analysis (GSA) described in High Accuracy Computing Methods, T.K. Sengupta, Cambridge Univ. Press, USA. The focus is on the second order Adams-Bashforth (AB2) and the extrapolation in time (EXT2) methods. Careful distinction is made for the first time step at t = 0 by either Euler forward or four-stage, fourth order Runge-Kutta (RK4) time schemes. The latter is used to solve a benchmark aeroacoustic problem. Several one-dimensional wave propagation models are analyzed: pure advection and advection-diffUsion equations. Various spatial discretizations are discussed, including Fourier spectral method. Attention is paid to the presence of physical and numerical modes as noted in the quadratic equation obtained from the difference equation for the model 1D convection equation. It is shown that AB2 method is less stable and accurate than EXT2 method, with respect to numerical dissipation and dispersion. This is true for the methods, in which the physical mode dominates over the numerical mode. Presented analysis provides useful guide to analyze any three-time level methods. (C) 2017 Elsevier Inc. All rights reserved.
引用
收藏
页码:41 / 57
页数:17
相关论文
共 50 条
[1]  
[Anonymous], 1990, "Numerical Computation of Internal and External Flows"
[2]  
[Anonymous], HIGH ORDER METHOD IN
[3]  
[Anonymous], 1999, Texts in Applied Mathematics
[4]  
[Anonymous], 1883, An Attempt to Test the Theories of Capillary Action by Comparing the Theoretical and Measured Forms of Drops of Fluid
[5]   A new velocity-vorticity formulation for direct numerical simulation of 3D transitional and turbulent flows [J].
Bhaumik, Swagata ;
Sengupta, Tapan K. .
JOURNAL OF COMPUTATIONAL PHYSICS, 2015, 284 :230-260
[6]   A linear focusing mechanism for dispersive and non-dispersive wave problems [J].
Bhumkar, Yogesh G. ;
Rajpoot, Manoj K. ;
Sengupta, Tapan K. .
JOURNAL OF COMPUTATIONAL PHYSICS, 2011, 230 (04) :1652-1675
[7]   A numerical investigation on the effect of the inflow conditions on the self-similar region of a round jet [J].
Boersma, BJ ;
Brethouwer, G ;
Nieuwstadt, FTM .
PHYSICS OF FLUIDS, 1998, 10 (04) :899-909
[8]  
BONTOUX P, 1978, J MEC APPL, V2, P291
[9]   Computational performance of a parallelized three-dimensional high-order spectral element toolbox [J].
Bosshard, Christoph ;
Bouffanais, Roland ;
Deville, Michel ;
Gruber, Ralf ;
Latt, Jonas .
COMPUTERS & FLUIDS, 2011, 44 (01) :1-8
[10]   Reynolds number effects on Rayleigh-Taylor instability with possible implications for type-Ia supernovae [J].
Cabot, William H. ;
Cook, Andrew W. .
NATURE PHYSICS, 2006, 2 (08) :562-568