铀高压状态方程的第一原理研究

张其黎 赵艳红 马桂存 张弓木

张其黎, 赵艳红, 马桂存, 张弓木. 铀高压状态方程的第一原理研究[J]. 高压物理学报, 2016, 30(1): 32-36. doi: 10.11858/gywlxb.2016.01.005
引用本文: 张其黎, 赵艳红, 马桂存, 张弓木. 铀高压状态方程的第一原理研究[J]. 高压物理学报, 2016, 30(1): 32-36. doi: 10.11858/gywlxb.2016.01.005
ZHANG Qi-Li, ZHAO Yan-Hong, MA Gui-Cun, ZHANG Gong-Mu. First-Principles Study of the Equation of Statefor Uranium under High Pressures[J]. Chinese Journal of High Pressure Physics, 2016, 30(1): 32-36. doi: 10.11858/gywlxb.2016.01.005
Citation: ZHANG Qi-Li, ZHAO Yan-Hong, MA Gui-Cun, ZHANG Gong-Mu. First-Principles Study of the Equation of Statefor Uranium under High Pressures[J]. Chinese Journal of High Pressure Physics, 2016, 30(1): 32-36. doi: 10.11858/gywlxb.2016.01.005

铀高压状态方程的第一原理研究

doi: 10.11858/gywlxb.2016.01.005
基金项目: 

国家自然科学基金 11102026

详细信息
    作者简介:

    张其黎(1972-), 男, 博士, 副研究员, 主要从事材料物性研究.E-mail:zhang_qili@iapcm.ac.cn

  • 中图分类号: O521.2

First-Principles Study of the Equation of Statefor Uranium under High Pressures

  • 摘要: 利用基于密度泛函理论的赝势平面波方法,研究了铀的状态方程。基态计算结果表明:在100GPa的压强范围内,α-U结构是最稳定的相。利用量子分子动力学方法(QMD),计算了有限温度下的状态方程,在此基础上计算了冲击Hugoniot点,并与实验数据及其他理论计算结果进行了比较,结果表明:在100GPa以下的压力区域内,QMD计算结果与实验结果符合得很好,而用快速计算状态方程(QEOS)方法计算的结果偏软。

     

  • 图  不同结构铀的原子总能与原子体积的关系

    Figure  1.  Total atomic energies vs.atomic volumesfor various structures of uranium

    图  不同结构铀的冷压与原子体积的关系

    Figure  2.  Cold pressures vs.atomic volumesfor various structures of uranium

    图  采用QMD方法计算的300K等温线

    Figure  3.  Isotherm at 300K calculated by QMD method

    图  铀的us-up关系曲线

    Figure  4.  us vs.up curves for uranium

    图  铀的压强-密度曲线

    Figure  5.  Pressure vs.density curves for uranium

  • [1] GANGULY J, KENNEDY G C.The melting temperature of uranium at high pressures[J]. J Phys Chem Solids, 1973, 34(12):2272-2274. doi: 10.1016/S0022-3697(73)80077-0
    [2] AKELLA J, SMITH G S, GROVER R, et al.Static EOS of uranium to 100 GPa pressure[J]. High Pressure Res, 1990, 2(5/6):295-302. doi: 10.1080/08957959008203182
    [3] YOO C S, AKELLA J, MORIARTY J A.High-pressure melting temperatures of uranium:laser-heating experiments and theoretical calculations[J]. Phys Rev B, 1993, 48(21):15529-15534. doi: 10.1103/PhysRevB.48.15529
    [4] AKELLA J, WEIR S, WILLS J M, et al.Structural stability in uranium[J]. J Phys Condens Matter, 1997, 9:L549-L555. doi: 10.1088/0953-8984/9/39/003
    [5] YOO C S, CYNN H, SODERLIND P.Phase diagram of uranium at high pressures and temperatures[J]. Phys Rev B, 1998, 57(17):10359-10362. doi: 10.1103/PhysRevB.57.10359
    [6] WYCKOFF R W G.Crystal structures[M]. New York:Interscience Publishers, 1963:16.
    [7] DEWAELE A, BOUCHET J, OCCELLI F, et al.Refinement of the equation of state of α-uranium[J]. Phys Rev B, 2013, 88(13):134202. doi: 10.1103/PhysRevB.88.134202
    [8] MARSH S P.LASL shock Hugoniot data[M]. Los Angeles, USA:University of California Press, 1980.
    [9] SKIDMORE I C, MORRIS E.Experimental equation-of-state data for uranium and its interpretation in the critical region[M]//Thermodynamics of nuclear materials.Vienna: International Atomic Energy Agency, 1962: 173-216.
    [10] ISBELL W M, SHIPMAN F H, JONES A H.Hugoniot equation of state measurements for eleven materials to five megabars: AD721920[R]. Warren, Michigan: Materials & Structures Laboratory, 1968.
    [11] JONES M D, BOETTGER J C, ALBERS R C.Theoretical atomic volumes of the light actinides[J]. Phys Rev B, 2000, 61(7):4644-4650. doi: 10.1103/PhysRevB.61.4644
    [12] SODERLIND P, ERIKSSON O, JOHANSSON B, et al.Electronic properties of f-electron metals using the generalized gradient approximation[J]. Phys Rev B, 1994, 50(11):7291-7294. doi: 10.1103/PhysRevB.50.7291
    [13] PENICAUD M.Calculated equilibrium properties, electronic structures and structural stabilities of Th, Pa, U, Np and Pu[J]. J Phys Condens Matter, 2000, 12(27):5819-5829. doi: 10.1088/0953-8984/12/27/301
    [14] SODERLIND P.First-principles elastic and structural properties of uranium metal[J]. Phys Rev B, 2002, 66(8):085113. doi: 10.1103/PhysRevB.66.085113
    [15] SODERLIND P, LANDA A, SADIGH B.First-principles elastic constants and phonons of δ-Pu[J]. Phys Rev B, 2004, 70(14):144103. doi: 10.1103/PhysRevB.70.144103
    [16] HOOD R Q, YANG L H, MORIARTY J A.Quantum molecular dynamics simulations of uranium at high pressure and temperature[J]. Phys Rev B, 2008, 78(2):024116. doi: 10.1103/PhysRevB.78.024116
    [17] MORE R M, WARREN K H, YOUNG D A, et al.A new quotidian equation of state (QEOS) for hot dense matter[J]. Phys Fluids, 1988, 31(10):3059-3078. doi: 10.1063/1.866963
  • 加载中
图(5)
计量
  • 文章访问数:  6912
  • HTML全文浏览量:  2841
  • PDF下载量:  123
出版历程
  • 收稿日期:  2014-10-09
  • 修回日期:  2014-12-29

目录

    /

    返回文章
    返回