C.N.R.S., Université Pierre et Marie Curie-Paris 6, Laboratoire de Physique Théorique de la Matière Condensée, UMR 7600, 4, Place Jussieu, case courrier 121, 75252 Paris cedex 05, France.
J Chem Phys. 2011 Jan 21;134(3):034121. doi: 10.1063/1.3522878.
We perform microscopic simulations using the direct simulation Monte Carlo approach to an exothermic chemical wave front of Fisher-Kolmogorov, Petrovsky, Piskunov-type in a one-dimensional gaseous medium. The results confirm the existence of a transition from a weak detonation or deflagration to a Chapman-Jouguet detonation wave, that we already investigated at the macroscopic scale [G. Dumazer et al., Phys. Rev. E 78, 016309 (2008)]. In the domain of weak detonation or deflagration, the discrepancy between the propagation speeds deduced from the simulations and the macroscopic balance equations of hydrodynamics is explained by two microscopic effects, the discretization of the variables, known as cutoff effect, and the departure from local equilibrium. Remarkably, the propagation speed of a Chapman-Jouguet detonation wave is not sensitive to these perturbations of microscopic origin.
我们使用直接模拟蒙特卡罗方法对一维气态介质中费舍尔-科尔莫戈罗夫、彼得罗夫斯基、皮斯库诺夫型的放热化学波前进行微观模拟。结果证实了存在从弱爆轰或爆燃到Chapman-Jouguet 爆轰波的转变,我们已经在宏观尺度上进行了研究[G. Dumazer 等人,Phys. Rev. E 78, 016309 (2008)]。在弱爆轰或爆燃的范围内,从模拟得出的传播速度与流体动力学宏观平衡方程之间的差异可以用两个微观效应来解释,即变量的离散化,称为截止效应,以及偏离局部平衡。值得注意的是,Chapman-Jouguet 爆轰波的传播速度对这些微观起源的扰动不敏感。