Two Complete Equations of State for Several Materials
-
摘要: 在一定程度上,状态方程的形式与外推数据的置信度有直接影响,对于在高压下发生反应的材料,通过外推方式计算其未反应状态具有一定的意义。依据由Vinet以及Parsafar和Mason(简称P-M)等人提出的两种统一状态方程,对以其为等温压缩线的完全状态方程进行了研究。根据对热力学状态量的分析,从热压系数和定容比热入手,对完全状态方程的建立进行了讨论,给出了在已知物质等温线条件下构成状态方程的方法,并推导了Vinet和P-M两种表达式的完全状态方程形式。以几种材料为例,通过实验测量的冲击绝热线和有关参数,采用最小二乘法,对其状态方程进行了拟合。结果表明,由冲击绝热线拟合的状态方程与实验结果相吻合。Abstract: This paper describes the formulation of the complete equation of state (EOS) for several materials, based on two universal EOS, proposed by Vinet et al, as well as Parsafar & Mason.And we discussed the formulation of the EOS from the thermal mechanics state expressed by thermal-pressure coefficient and specific heat coefficient.Finally, we fitted the obtained EOS with those obtained shock wave data from references by linear fitting method.The calculated shock Hugoniot state from the obtained two complete EOS are compared with shock Hugoniot data, and good agreements are showed.
-
Key words:
- equation of state /
- unrected explosive /
- shock Hugoniot /
- thermomechanics compatibility
-
表 1 统一物态方程的计算输入参数
Table 1. JWL EOS Parameters of explosives
表 2 几种材料物态方程参数的拟合结果
Table 2. Fitted EOS parameters of several materials
Materials ρ0/(g/cm3) P-M EOS parameters Vinet EOS parameters A0/10-3 A1/10-3 A2/10-3 B0/10-3 η/10-2 Θ/10-7 JB-9014 1.887 -108.562 98.071 2 10.490 8 123.184 644.764 84.915 PBX-9404 1.867 70.899 3 -240.205 169.306 126.329 944.389 50.409 45 steel 7.85 -378.596 -270.837 649.434 1 087.32 822.45 769.959 Tungsten 19.2 -4 248.49 5 473.94 -1 225.45 3 110.78 443.387 414.487 -
[1] Murnaghan F D. The Compressibility of media under extreme pressures[J]. PNAS, 1944, 30(9): 244-247. doi: 10.1073/pnas.30.9.244 [2] Dymond J H, Malhotra R. The Tait equation: 100 years on[J]. Int J Thermophys, 1988, 9(6): 941-951. doi: 10.1007/BF01133262 [3] Birch F. Finite elastic strain of cubic crystals[J]. Phys Rev, 1947, 71: 809. doi: 10.1103/PhysRev.71.809 [4] Birch F. Finite strain isotherm and velocities for single-crystal and polycrystalline NaCl at high pressures and 300 K[J]. J Geophys Res: Solid Earth, 1978, 83(B3): 1257-1268. doi: 10.1029/JB083iB03p01257 [5] Gholamabbas Parsafar, Mason E A. Universal equation of state for compressed solids[J]. Phys Rev B, 1994, 49(5): 3049-3060. doi: 10.1103/PhysRevB.49.3049 [6] Macdonald J R. Review of some experimental and analytical equations of state[J]. Rev Mod Phys, 1969, 41: 316. doi: 10.1103/RevModPhys.41.316 [7] Vinet P, Ferrante J, Smith J R, et al. An universal equation of state for solids[J]. J Phys C: Solid State Phys, 1986, 19(20): L467-L473. doi: 10.1088/0022-3719/19/20/001 [8] Vinet P, Ferrante J, Rose J H, et al. Compressibility of solids[J]. J Geophys Res, 1987, 92(B9): 9319-9325. doi: 10.1029/JB092iB09p09319 [9] Vinet P, Smith J R, Ferrante J, et al. Temperature effects on the universal equation of state of solids[J]. Phys Rev B, 1987, 35(4): 1945. doi: 10.1103/PhysRevB.35.1945 [10] Walsh J M, Rice M H, McQueen R G, et al. Shock-wave compressions of twenty-seven metals. Equations of state of metals[J]. Phys Rev, 1957, 108: 196. doi: 10.1103/PhysRev.108.196 [11] Steinberg D J. Equation of state and strength properties of selected materials, UCRL-MA-106439[R]. Livermore: Lawrence Livermore National Laboratory, 1991. [12] Mader C L. Numerical Modeling of Detonation[M]. California: University of California Press, 1979. [13] Marsh S P. LASL Shock Hugoniot Data[M]. California: University of California Press, 1980. [14] 王青松. 45钢冲击绝热线参数测量[R].绵阳: 中国工程物理研究院流体物理研究所, 2004.Wang Q S. Measurement of shock Hugoniot parameters of 45 steel[R]. Mianyang: Institute of Fluid Physics, CAEP, 2004. (in Chinese) [15] Los Alamos National Laboratory. Selected Hugoniots, LA-4167-MS[R]. New Mexico: Los Alamos National Laboratory, 1969. [16] 赵锋.炸药强爆轰驱动高速金属飞片的实验和理论研究[D].绵阳: 中国工程物理研究院研究生部, 2005.Zhao F. Research on high speed metal flyer accerated by strong detonation of explosives[D]. Mianyang: Graduate School, CAEP, 2005. (in Chinese)