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作 者:ZHANG Xiao-Qiang WANG Guang-Rui CHEN Shi-Gang
机构地区:[1]Department of Physics, Hebei Normal University, Shijiazhuang 050016, China [2]Graduate School of the China Academy of Engineering Physics, P.O. Box 8009(28), Beijing 100088, China [3]Center for Nonlinear Studies, Institute of Applied Physics and Computational Mathematics, Beijing 100088, China
出 处:《Communications in Theoretical Physics》2008年第4期1033-1038,共6页理论物理通讯(英文版)
基 金:The project supported by National Natural Science Foundation for Major Projects under Grant Nos.10336010 and 10576005
摘 要:A shell-model version of passive scalar problem is introduced, which is inspired by the model of K. Ohkitani and M. Yakhot [K. Ohkitani and M. Yakhot, Phys. Rev. Lett. 60 (1988) 983; K. Ohkitani and M. Yakhot, Prog. Theor. Phys. 81 (1988) 329]. As in the original problem, the prescribed random velocity field is Gaussian and 5 correlated in time. Deterministic differential equations are regarded as nonlinear Langevin equation. Then, the Fokker-Planck equations of PDF for passive scalars are obtained and solved numerically. In energy input range (n 〈 5, n is the shell number.), the probability distribution function (PDF) of passive scalars is near the Gaussian distribution. In inertial range (5≤ n ≤ 16) and dissipation range (n ≥ 17), the probability distribution function (PDF) of passive scalars has obvious intermittence. And the scaling power of passive scalar is anomalous. The results of numerical simulations are compared with experimental measurements.
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