The Thermal Conductivity of Magnesite, Dolomite and Calcite as Determined by Molecular Dynamics Simulation

Leila Momenzadeh, B. Moghtaderi, X. Liu, S. Sloan, I. Belova, G. Murch
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引用次数: 10

Abstract

In this study, the phonon-based thermal conductivity of magnesite (MgCO3) and dolomite (CaMg(CO3)2) is calculated and compared with an earlier recent calculation on calcite (CaCO3). Equilibrium molecular dynamics simulation by way of the elegant Green-Kubo formalism is used for calculating the thermal conductivity. The thermal conductivity is investigated over a wide temperature range (from 200 K to 800 K) for all of the above mentioned materials. The most reliable potential parameters are used for characterising the interatomic interactions. In all of the models, two independent mechanisms are considered. The first is temperature independent, which is relevant to the acoustic short-range and optical phonons, and the other is temperature dependent, which is linked to the acoustic long-range phonons. In the study, the heat current autocorrelation function (HCACF) is calculated over the averages of the NPT, NVT and NVE ensembles in the x- and z- directions. In addition, it is shown that the optical, acoustic short- and long-range phonon modes are the main contributors to the decomposition model of the thermal conductivity. In a further investigation, the effects of the computational cell sizes on the thermal conductivity are investigated with five different simulation blocks containing 30, 240, 810, 1920 and 6480 atoms. Finally, this research provides a comparison of the thermal conductivity from this study and experimental studies: they are in good agreement.
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用分子动力学模拟测定菱镁矿、白云石和方解石的导热性
本研究计算了菱镁矿(MgCO3)和白云石(CaMg(CO3)2)的声基导热系数,并与近期方解石(CaCO3)的计算结果进行了比较。采用优雅的Green-Kubo形式进行平衡分子动力学模拟,计算导热系数。在较宽的温度范围内(从200 K到800 K)对所有上述材料的导热性进行了研究。最可靠的势参数被用来描述原子间的相互作用。在所有的模型中,都考虑了两个独立的机制。第一种是与温度无关的,这与声学短程声子和光学声子有关,另一种是与温度相关的,这与声学远程声子有关。在研究中,热流自相关函数(HCACF)计算了在x和z方向上NPT、NVT和NVE系综的平均值。此外,光学、声学短、远程声子模式是热导率分解模型的主要贡献者。在进一步的研究中,研究了计算单元尺寸对导热系数的影响,采用了包含30、240、810、1920和6480个原子的五种不同的模拟块。最后,将本研究所得的导热系数与实验结果进行了比较,结果吻合较好。
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