Numerical simulation of interaction of the heavy gas cloud with the atmospheric surface layer

被引:21
作者
Kovalets, I. V. [1 ]
Maderich, V. S. [1 ]
机构
[1] Inst Math Machine & Syst Problems, UA-03187 Kiev, Ukraine
关键词
heavy gas dispersion; mixed convection; Richardson number; splitting methods and stratified flows;
D O I
10.1007/s10652-005-4288-4
中图分类号
X [环境科学、安全科学];
学科分类号
08 [工学]; 0830 [环境科学与工程];
摘要
The numerical time-dependent three-dimensional model [Kovalets, I.V. and Maderich, V.S.: 2001, Int. J. Fluid Mech. Res. 30, 410-429] of the heavy gas dispersion in the atmospheric boundary layer has been improved by parameterizing momentum and heat fluxes on the surface of Earth using Monin-Obukhov similarity theory. Three parameterizations of heat exchange with the surface of Earth were considered: (A) formula of Yaglom A.M. and Kader B.A. [1974, J. Fluid Mech. 62, 601-623] for forced convection, (B) interpolation formula for mixed convection and (C) similarity relationship for mixed convection [Kader, B.A. and Yaglom, A.M.: 1990, J. Fluid Mech. 212, 637-662]. Two case studies were considered. In the first study based on experiment of Zhu et al., J. Hazard Mater 62, 161-186], the interaction of an isothermal heavy gas plume with an atmospheric surface layer was simulated. It was found that stable stratification in the cloud essentially suppresses the turbulence in the plume, reducing the turbulent momentum flux by a factor of down to 1/5 in comparison with the undisturbed value. This reduction essentially influences velocities in the atmospheric boundary layer above the cloud, increasing the mean velocity by a factor of up to 1.3 in comparison with the undisturbed value. A simulation of cold heavy gas dispersion was carried out in the second case based on field experiment BURRO 8. It was shown that both forced and free convections under moderate wind speeds significantly influence the plume. The relative rms and bias errors of prediction the plume's height were sigma(H) approximate to 30% and epsilon(H) = -10%, respectively, for parameterization B, while for A and C the errors were sigma(H) approximate to 80% and epsilon(H) approximate to -65%. It is therefore advised to use the simple parameterization B in dense gas dispersion models.
引用
收藏
页码:313 / 340
页数:28
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