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On the domain size effect of thermal conductivities from equilibrium and nonequilibrium molecular dynamics simulations

机译:通过平衡和非平衡分子动力学模拟研究热导率的畴尺寸效应

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摘要

Equilibrium molecular dynamics (EMD) simulations with the Green-Kubo formula and nonequilibrium molecular dynamics (NEMD) simulations with the Fourier's Law are two widely used methods for calculating thermal conductivities of materials. It is well known that both methods suffer from domain size effects, especially for NEMD. But the underlying mechanisms and their comparison have not been much quantitatively studied before. In this paper, we investigate their domain size effects by using crystalline silicon at 1000 K, graphene at 300 K, and silicene at 300 K as model material systems. The thermal conductivity of silicon from EMD simulations increases normally with the increasing domain size and converges at a size of around 4×4×4 nm~3. The converging trend agrees well with the wavelength-accumulated thermal conductivity. The thermal conductivities of graphene and silicene from EMD simulations decrease abnormally with the increasing domain size and converge at a size of around 10 × 10nm~2. We ascribe the anomalous size effect to the fact that as the domain size increases, the effect of more phonon scattering processes (particularly the flexural phonons) dominates over the effect of more phonon modes contributing to the thermal conductivity. The thermal conductivities of the three material systems from NEMD simulations all show normal domain size effects, although their dependences on the domain size differ. The converging trends agree with the mean free path accumulation of thermal conductivity. This study provides new insights that other than some exceptions, the domain size effects of EMD and NEMD are generally associated with wavelength and mean free path accumulations of thermal conductivity, respectively. Since phonon wavelength spans over a much narrower range than mean free path, EMD usually has less significant domain size effect than NEMD.
机译:使用Green-Kubo公式进行的平衡分子动力学(EMD)模拟和使用傅立叶定律的非平衡分子动力学(NEMD)模拟是计算材料导热系数的两种广泛使用的方法。众所周知,两种方法都受到域大小影响,尤其是对于NEMD。但是,其潜在机理及其​​比较尚未进行过定量的研究。在本文中,我们通过使用1000 K的结晶硅,300 K的石墨烯和300 K的硅酮作为模型材料系统研究它们的畴尺寸效应。 EMD模拟得出的硅的导热系数通常随着畴尺寸的增加而增加,并收敛在4×4×4 nm〜3左右的尺寸。会聚趋势与波长累积的热导率非常吻合。 EMD模拟中石墨烯和硅的热导率随畴尺寸的增加而异常降低,并收敛在10×10nm〜2左右。我们将异常尺寸效应归因于以下事实:随着畴尺寸的增加,更多的声子散射过程(尤其是挠曲声子)的影响将主导更多的声子模式对导热性的影响。来自NEMD模拟的三种材料系统的热导率均显示出正常的畴尺寸效应,尽管它们对畴尺寸的依赖性不同。收敛趋势与热导率的平均自由程累积一致。这项研究提供了新的见解,除某些例外外,EMD和NEMD的域尺寸效应通常分别与波长和导热系数的平均自由程累积有关。由于声子波长的跨度比平均自由程窄得多,因此EMD通常不如NEMD那么显着。

著录项

  • 来源
    《Journal of Applied Physics》 |2017年第4期|044301.1-044301.8|共8页
  • 作者

    Zuyuan Wang; Xiulin Ruan;

  • 作者单位

    School of Mechanical Engineering and the Birck Nanotechnology Center, Purdue University, West Lafayette, Indiana 47907, USA;

    School of Mechanical Engineering and the Birck Nanotechnology Center, Purdue University, West Lafayette, Indiana 47907, USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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