Temperature decay in two-phase turbulent flows

被引:32
作者
Jaberi, FA [1 ]
Mashayek, F
机构
[1] Kansas State Univ, Dept Mech & Nucl Engn, Manhattan, KS 66506 USA
[2] Univ Hawaii Manoa, Dept Mech Engn, Honolulu, HI 96822 USA
关键词
two-phase turbulent flows; thermal transport; direct numerical simulations;
D O I
10.1016/S0017-9310(99)00185-4
中图分类号
O414.1 [热力学];
学科分类号
摘要
Direct numerical simulations of dilute two-phase flows are conducted to study the decay of the fluid and particle temperatures in isotropic turbulence. Both one-way and two-way couplings between phases are considered. The effects of the particle response time (tau(p)), the Prandtl number (Pr), the ratio of specific heats (alpha), and the mass loading ratio (phi(m)) on the carrier fluid and particle temperature statistics are studied. The results indicate that the variance of the fluid and particle temperatures, the dissipation rate of the fluid temperature and the high wavenumber values of the fluid temperature spectrum are increased as the magnitudes of phi(m) and/or alpha Pr increase. The decay rate of the fluid and particle temperature variances an similar when the values of alpha Pr are small. For large alpha Pr values, the variance of the particle temperature is higher than that of the fluid and is strongly dependent on the initial conditions. The Lagrangian auto-correlation coefficient of the particle temperature (R-T(p)) also behaves differently for different magnitudes of alpha and Pr. For small values of alpha, R-T(p) decreases as the magnitude of particle response time increases. For large values of alpha, R-T(p) increases with increasing tau(p). (C) 2000 Elsevier Science Ltd. All rights reserved.
引用
收藏
页码:993 / 1005
页数:13
相关论文
共 33 条
[1]  
[Anonymous], 1990, TURBULENT FLOWS GAS
[2]   DIFFUSION IN A FIELD OF HOMOGENEOUS TURBULENCE .2. THE RELATIVE MOTION OF PARTICLES [J].
BATCHELOR, GK .
PROCEEDINGS OF THE CAMBRIDGE PHILOSOPHICAL SOCIETY, 1952, 48 (02) :345-362
[3]   PARTICLE MIXING IN FREE SHEAR FLOWS [J].
CROWE, CT ;
CHUNG, JN ;
TROUTT, TR .
PROGRESS IN ENERGY AND COMBUSTION SCIENCE, 1988, 14 (03) :171-194
[4]   PARTICLE-SOURCE IN CELL (PSI-CELL) MODEL FOR GAS-DROPLET FLOWS [J].
CROWE, CT ;
SHARMA, MP ;
STOCK, DE .
JOURNAL OF FLUIDS ENGINEERING-TRANSACTIONS OF THE ASME, 1977, 99 (02) :325-332
[5]   Numerical models for two-phase turbulent flows [J].
Crowe, CT ;
Troutt, TR ;
Chung, JN .
ANNUAL REVIEW OF FLUID MECHANICS, 1996, 28 :11-43
[6]  
CSANADY GT, 1963, J ATMOS SCI, V20, P201, DOI 10.1175/1520-0469(1963)020<0201:TDOHPI>2.0.CO
[7]  
2
[8]   PREFERENTIAL CONCENTRATION OF PARTICLES BY TURBULENCE [J].
EATON, JK ;
FESSLER, JR .
INTERNATIONAL JOURNAL OF MULTIPHASE FLOW, 1994, 20 :169-209
[9]   ON THE 2-WAY INTERACTION BETWEEN HOMOGENEOUS TURBULENCE AND DISPERSED SOLID PARTICLES .1. TURBULENCE MODIFICATION [J].
ELGHOBASHI, S ;
TRUESDELL, GC .
PHYSICS OF FLUIDS A-FLUID DYNAMICS, 1993, 5 (07) :1790-1801
[10]   AN EXAMINATION OF FORCING IN DIRECT NUMERICAL SIMULATIONS OF TURBULENCE [J].
ESWARAN, V ;
POPE, SB .
COMPUTERS & FLUIDS, 1988, 16 (03) :257-278