HYDRODYNAMIC DISPERSION AT STAGNATION POINTS - SIMULATIONS AND EXPERIMENTS

被引:60
作者
FLEKKOY, EG
OXAAL, U
FEDER, J
JOSSANG, T
机构
[1] NORWEGIAN ACAD SCI & LETTERS,CTR ADV STUDY,N-0205 OSLO,NORWAY
[2] UNIV OSLO,DEPT PHYS,N-0316 OSLO,NORWAY
来源
PHYSICAL REVIEW E | 1995年 / 52卷 / 05期
关键词
D O I
10.1103/PhysRevE.52.4952
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
The spreading of a passive tracer that is convected back and forth inside a porous medium depends both on the random characteristics of the medium and on the presence of stagnation points. We single out the effect of the latter in the present study of hydrodynamic dispersion in the creeping (low Reynolds number) high Peclet number how around the single stagnation point on a cylindrical obstacle in a Hele-Shaw cell [U. Oxaal, E. G. Flekkoy, and J. Feder, Phys. Rev. Lett. 72, 3514 (1994)]. Employing both experiments and lattice Boltzmann simulations we analyze the dispersive spreading of a single tracer line, which is initially perpendicular to the how direction and then convected back and forth around the cylinder. The lattice Boltzmann model used is a modification of the recently introduced two-dimensional lattice Bhatnagar-Gross-Krook model for miscible fluid dynamics [E. G. Flekkoy, Phys. Rev. E 47, 4247 (1993)]. It includes the full three-dimensional viscous interaction in the Hele-Shaw cell and, in the case of steady state how, it allows for a freely tunable Reynolds number. The diffusive behavior of the system is explored extensively and excellent agreement between simulations and experiment is observed. A method to determine very small molecular diffusion coefficients D, which relies on the combination of results from experiment and simulation, is proposed. It is demonstrated that there is good agreement between the result of this method and independent measurements that are carried out in the present case of relatively large D values.
引用
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页码:4952 / 4962
页数:11
相关论文
共 20 条
[1]  
BATCHELOR G. K., 1970, INTRO FLUID DYNAMICS
[2]  
BAUDET C, 1985, J PHYS LETT, V46, pL991
[3]  
Doolen G. D., 1990, LATTICE GAS METHODS
[4]   LATTICE BHATNAGAR-GROSS-KROOK MODELS FOR MISCIBLE FLUIDS [J].
FLEKKOY, EG .
PHYSICAL REVIEW E, 1993, 47 (06) :4247-4257
[5]   LATTICE-GAS AUTOMATA FOR THE NAVIER-STOKES EQUATION [J].
FRISCH, U ;
HASSLACHER, B ;
POMEAU, Y .
PHYSICAL REVIEW LETTERS, 1986, 56 (14) :1505-1508
[6]   A LATTICE-GAS MODEL FOR 3 IMMISCIBLE FLUIDS [J].
GUNSTENSEN, AK ;
ROTHMAN, DH .
PHYSICA D, 1991, 47 (1-2) :47-52
[7]  
GUYON E, 1988, DISORDER MIXING
[8]  
HIBY JW, 1962, P S INTERACTIONS FLU, P312
[9]   SIMULATING THE FLOW AROUND A CIRCULAR-CYLINDER WITH A LATTICE BOLTZMANN-EQUATION [J].
HIGUERA, FJ ;
SUCCI, S .
EUROPHYSICS LETTERS, 1989, 8 (06) :517-521
[10]   LATTICE-GAS AND LATTICE-BOLTZMANN MODELS OF MISCIBLE FLUIDS [J].
HOLME, R ;
ROTHMAN, DH .
JOURNAL OF STATISTICAL PHYSICS, 1992, 68 (3-4) :409-429