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温稠密铍的状态方程和输运性质:量子分子动力学研究

Equations of state and transport properties of warm dense beryllium: a quantum molecular dynamics study.

作者信息

Wang Cong, Long Yao, Tian Ming-Feng, He Xian-Tu, Zhang Ping

机构信息

Institute of Applied Physics and Computational Mathematics, P.O. Box 8009, Beijing 100088, People's Republic of China.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Apr;87(4):043105. doi: 10.1103/PhysRevE.87.043105. Epub 2013 Apr 12.

Abstract

We have calculated the equations of state, the viscosity and self-diffusion coefficients, and electronic transport coefficients of beryllium in the warm dense regime for densities from 4.0 to 6.0 g/cm(3) and temperatures from 1.0 to 10.0 eV by using quantum molecular dynamics simulations. The principal Hugoniot curve is in agreement with underground nuclear explosive and high-power laser experimental results up to ~20 Mbar. The calculated viscosity and self-diffusion coefficients are compared with the one-component plasma model, using effective charges given by the average-atom model. The Stokes-Einstein relationship, which connects viscosity and self-diffusion coefficients, is found to hold fairly well in the strong coupling regime. The Lorenz number, which is the ratio between thermal and electrical conductivities, is computed via Kubo-Greenwood formula and compared to the well-known Wiedemann-Franz law in the warm dense region.

摘要

我们通过量子分子动力学模拟计算了密度在4.0至6.0 g/cm³、温度在1.0至10.0 eV的温稠密区域内铍的状态方程、粘度和自扩散系数以及电子输运系数。主雨贡纽曲线与地下核爆炸和高功率激光实验结果在高达约20 Mbar时一致。使用平均原子模型给出的有效电荷,将计算得到的粘度和自扩散系数与单组分等离子体模型进行了比较。发现连接粘度和自扩散系数的斯托克斯-爱因斯坦关系在强耦合区域相当适用。通过久保-格林伍德公式计算了热导率与电导率之比的洛伦兹数,并在温稠密区域将其与著名的维德曼-夫兰兹定律进行了比较。

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