Technique for forcing high Reynolds number isotropic turbulence in physical space

被引:14
作者
Palmore, John A., Jr. [1 ]
Desjardins, Olivier [1 ]
机构
[1] Cornell Univ, Sibley Sch Mech & Aerosp Engn, Ithaca, NY 14853 USA
来源
PHYSICAL REVIEW FLUIDS | 2018年 / 3卷 / 03期
基金
美国国家科学基金会;
关键词
DIRECT NUMERICAL SIMULATIONS; HOMOGENEOUS TURBULENCE; SCHEME; FLOWS;
D O I
10.1103/PhysRevFluids.3.034605
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Many common engineering problems involve the study of turbulence interaction with other physical processes. For many such physical processes, solutions are expressed most naturally in physical space, necessitating the use of physical space solutions. For simulating isotropic turbulence in physical space, linear forcing is a commonly used strategy because it produces realistic turbulence in an easy-to-implement formulation. However, the method resolves a smaller range of scales on the same mesh than spectral forcing. We propose an alternative approach for turbulence forcing in physical space that uses the low-pass filtered velocity field as the basis of the forcing term. This method is shown to double the range of scales captured by linear forcing while maintaining the flexibility and low computational cost of the original method. This translates to a 60% increase of the Taylor microscale Reynolds number on the same mesh. An extension is made to scalar mixing wherein a scalar field is forced to have an arbitrarily chosen, constant variance. Filtered linear forcing of the scalar field allows for control over the length scale of scalar injection, which could be important when simulating scalar mixing.
引用
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页数:18
相关论文
共 32 条
[1]   Random forcing of three-dimensional homogeneous turbulence [J].
Alvelius, K .
PHYSICS OF FLUIDS, 1999, 11 (07) :1880-1889
[2]   Constant-energetics physical-space forcing methods for improved convergence to homogeneous-isotropic turbulence with application to particle-laden flows [J].
Bassenne, Maxime ;
Urzay, Javier ;
Park, George I. ;
Moin, Parviz .
PHYSICS OF FLUIDS, 2016, 28 (03)
[3]  
BICKLEY WG, 1948, Q J MECH APPL MATH, V1, P33
[4]   A proposed modification to Lundgren's physical space velocity forcing method for isotropic turbulence [J].
Carroll, Phares L. ;
Blanquart, G. .
PHYSICS OF FLUIDS, 2013, 25 (10)
[5]   A novel forcing technique to simulate turbulent mixing in a decaying scalar field [J].
Carroll, Phares L. ;
Verma, Siddhartha ;
Blanquart, G. .
PHYSICS OF FLUIDS, 2013, 25 (09)
[6]   ON STATISTICAL CORRELATIONS BETWEEN VELOCITY INCREMENTS AND LOCALLY AVERAGED DISSIPATION IN HOMOGENEOUS TURBULENCE [J].
CHEN, SY ;
DOOLEN, GD ;
KRAICHNAN, RH ;
SHE, ZS .
PHYSICS OF FLUIDS A-FLUID DYNAMICS, 1993, 5 (02) :458-463
[7]   Anisotropic linear forcing for synthetic turbulence generation in large eddy simulation and hybrid RANS/LES modeling [J].
de Meux, B. de Laage ;
Audebert, B. ;
Manceau, R. ;
Perrin, R. .
PHYSICS OF FLUIDS, 2015, 27 (03)
[8]   High order conservative finite difference scheme for variable density low Mach number turbulent flows [J].
Desjardins, Olivier ;
Blanquart, Guillaume ;
Balarac, Guillaume ;
Pitsch, Heinz .
JOURNAL OF COMPUTATIONAL PHYSICS, 2008, 227 (15) :7125-7159
[9]   Analysis of the clustering of inertial particles in turbulent flows [J].
Esmaily-Moghadam, Mahdi ;
Mani, Ali .
PHYSICAL REVIEW FLUIDS, 2016, 1 (08)
[10]   AN EXAMINATION OF FORCING IN DIRECT NUMERICAL SIMULATIONS OF TURBULENCE [J].
ESWARAN, V ;
POPE, SB .
COMPUTERS & FLUIDS, 1988, 16 (03) :257-278