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方解石与CaCO₃-II之间相变的分子动力学模拟

Molecular dynamics simulation of the phase transition between calcite and CaCO(3)-II.

作者信息

Kawano Jun, Miyake Akira, Shimobayashi Norimasa, Kitamura Masao

机构信息

Department of Earth and Planetary Science, Faculty of Science, Kyoto University, Kyoto 606-8502, Japan.

出版信息

J Phys Condens Matter. 2009 Jul 8;21(27):275403. doi: 10.1088/0953-8984/21/27/275403. Epub 2009 Jun 10.

DOI:10.1088/0953-8984/21/27/275403
PMID:21828487
Abstract

Molecular dynamics (MD) simulation of calcium carbonate at high pressure was performed to understand the phase transition between calcite [Formula: see text] and CaCO(3)-II (P 2(1)/c). In the 300-800 K temperature range, the transition of calcite to CaCO(3)-II was reproduced at a pressure of around 8 GPa. This transition is of first order and reversible in the MD calculations except for runs at 300 K where a small hysteresis exists. The slope of the dP/dT curve at the phase boundary between calcite and CaCO(3)-II is negative at 300 K and turns positive at around 600 K, which was confirmed by analyzing the enthalpy change. Just below the transition pressure, the P 2(1)/c structure appears and its orientation switches among three positions with time, resulting in the maintenance of the [Formula: see text] structure as a whole. The P 2(1)/c structure resembles the structure of CaCO(3)-II on an increase of temperature. It can be suggested that the existence of the P 2(1)/c structure and the switching of its orientation just below the transition pressure are responsible for the change of the slope of the dP/dT curve at the boundary from negative to positive on an increase of temperature, because the switching increases entropy and results in an expansion of the stability field of calcite.

摘要

为了理解方解石[化学式:见正文]与CaCO₃-II(P 2₁/c)之间的相变,进行了碳酸钙在高压下的分子动力学(MD)模拟。在300 - 800K的温度范围内,在约8GPa的压力下再现了方解石向CaCO₃-II的转变。除了在300K运行时存在小的滞后现象外,这种转变在MD计算中是一级且可逆的。通过分析焓变证实,方解石与CaCO₃-II相界处的dP/dT曲线斜率在300K时为负,在约600K时变为正。就在转变压力以下,P 2₁/c结构出现,其取向随时间在三个位置之间切换,从而整体上维持了[化学式:见正文]结构。随着温度升高,P 2₁/c结构类似于CaCO₃-II的结构。可以认为,P 2₁/c结构的存在及其在转变压力以下取向的切换导致了边界处dP/dT曲线斜率随温度升高从负变正,因为这种切换增加了熵并导致方解石稳定场的扩展。

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