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由共存的固液相计算得出的冰Ih的熔点。

Melting temperature of ice Ih calculated from coexisting solid-liquid phases.

作者信息

Wang J, Yoo S, Bai J, Morris James R, Zeng X C

机构信息

Department of Chemistry, University of Nebraska--Lincoln, 68588, USA.

出版信息

J Chem Phys. 2005 Jul 15;123(3):36101. doi: 10.1063/1.1950647.

Abstract

We carried out molecular-dynamics simulations by using the two-phase coexistence method with the constant pressure, particle number, and enthalpy ensemble to compute the melting temperature of proton-disordered hexagonal ice I(h) at 1-bar pressure. Four models of water were considered, including the widely used TIP4P [W. L. Jorgensen, J. Chandrasekha, J. D. Madura, R. W. Impey, and M. L. Klein, J. Chem. Phys.79, 926 (1983)] and TIP5P [M. W. Mahoney and W. L. Jorgensen J. Chem. Phys.112, 8910 (2000)] models, as well as recently improved TIP4P and TIP5P models for use with Ewald techniques-the TIP4P-Ew [W. Horn, W. C. Swope, J. W. Pitera, J. C. Madura, T. J. Dick, G. L. Hura, and T. Head-Gordon, J. Chem. Phys.120, 9665 (2004)] and TIP5P-Ew [S. W. Rick, J. Chem. Phys.120, 6085 (2004)] models. The calculated melting temperature at 1 bar is T(m) = 229 +/- 1 K for the TIP4P and T(m) = 272.0 +/- 0.6 K for the TIP5P ice I(h), both are consistent with previous simulations based on free-energy methods. For the TIP4P-Ew and TIP5P-Ew models, the calculated melting temperature is T(m) = 257.0 +/- 1.1 K and T(m) = 253.9 +/- 1.1 K, respectively.

摘要

我们采用恒压、粒子数和焓系综的两相共存方法进行分子动力学模拟,以计算1巴压力下质子无序六方冰I(h)的熔化温度。考虑了四种水模型,包括广泛使用的TIP4P [W. L. 乔根森、J. 钱德拉塞卡、J. D. 马杜拉、R. W. 英佩伊和M. L. 克莱因,《化学物理杂志》79, 926 (1983)] 和TIP5P [M. W. 马奥尼和W. L. 乔根森,《化学物理杂志》112, 8910 (2000)] 模型,以及最近改进的用于埃瓦尔德技术的TIP4P和TIP5P模型——TIP4P-Ew [W. 霍恩、W. C. 斯沃普、J. W. 皮特拉、J. C. 马杜拉、T. J. 迪克、G. L. 胡拉和T. 黑德-戈登,《化学物理杂志》120, 9665 (2004)] 和TIP5P-Ew [S. W. 里克,《化学物理杂志》120, 6085 (2004)] 模型。对于TIP4P,计算出的1巴下的熔化温度为T(m) = 229 ± 1 K,对于TIP5P冰I(h),T(m) = 272.0 ± 0.6 K,两者均与先前基于自由能方法的模拟结果一致。对于TIP4P-Ew和TIP5P-Ew模型,计算出的熔化温度分别为T(m) = 257.0 ± 1.1 K和T(m) = 253.9 ± 1.1 K。

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