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First-Principle Calculations of Collision Integrals for N_2-O System

机译:N_2-O系统碰撞积分的第一性原理计算

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Collision integrals related to viscosity and coefficient of diffusion are calculated by quasi-classical trajectory (QCT) method for N_2-O system. Three ab-initio potential energy surfaces (PES) for 1~1A', 1~3A' and 1~3A" electronic states are used. Contributions of inelastic collisions to collision integrals are taken into account by Wang-Chang and Uhlenbeck's theory. The results show that, collision integrals change by up to 20% for the two triplet states and 50% for the singlet state at vibrational nonequilibrium conditions. For conditions with |T - T_v| ≤ 5,000 K, the deviation of collisions integrals from their value at thermal equilibrium conditions is less than 5% and collision integrals, as well as transport coefficients, can be described by a single translational temperature. Compared with those obtained by using Lennard-Jones and exponential potential, the new results are within the uncertainty interval. By studying scattering angles, strong forward scattering is found at hyperthermal conditions, which implies that isotropic scattering law tends to overpredict transport properties. Phenomenological models like variable hard sphere (VHS) in direct simulation Monte Carlo (DSMC) become inaccurate for hyperthermal collisions. A new collision model is suggested based on the QCT results.
机译:通过N_2-O体系的准经典轨迹(QCT)方法计算了与黏度和扩散系数有关的碰撞积分。使用了三个电子初始势能面(PES),分别用于1〜1A',1〜3A'和1〜3A“电子态。Wang-Chang和Uhlenbeck的理论考虑了非弹性碰撞对碰撞积分的贡献。结果表明,在振动非平衡条件下,两个三重态的碰撞积分变化高达20%,而单重态的碰撞积分变化高达50%;对于| T-T_v |≤5,000 K的条件,碰撞积分偏离其值热平衡条件小于5%,并且碰撞积分以及传输系数可以用一个平移温度来描述,与使用Lennard-Jones和指数势所获得的结果相比,新结果在不确定区间内。研究散射角时,在高温条件下会发现强烈的正向散射,这表明各向同性散射定律倾向于高估输运性质。直接模拟中的硬球(VHS)蒙特卡洛(DSMC)对于过热碰撞变得不准确。根据QCT结果,提出了一种新的碰撞模型。

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