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Thermal Transport Mechanisms in Carbon Nanotube-Nanofluids Identified From Molecular Dynamics Simulations

机译:从分子动力学模拟确定碳纳米管-纳米流体中的热传递机理

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摘要

Atomistic simulations of carbon nanotubes (CNTs) in a liquid environment are performed to better understand thermal transport in CNT-based nanofluids. Thermal conductivity is studied using nonequilibrium molecular dynamics (MD) methods to understand the effective conductivity of a solvated CNT combined with a novel application of Hamilton-Grosser (HC) theory to estimate the conductivity of a fluid suspension of CNTs. Simulation results show how the presence of the fluid affects the CNTs ability to transport heat by disrupting the low-frequency acoustic phonons of the CNT. A spatially dependent use of the Irving-Kirkwood relations reveals the localized heat flux, illuminating the heat transfer pathways in the composite material. Model results can be consistently incorporated into HC theory by considering ensembles of CNTs and their surrounding fluid as being present in the liquid. The simulation-informed theory is shown to be consistent with existing experimental results.
机译:在液体环境中对碳纳米管(CNT)进行原子模拟,以更好地了解基于CNT的纳米流体中的热传输。使用非平衡分子动力学(MD)方法研究热导率,以了解溶剂化CNT的有效电导率,并结合Hamilton-Grosser(HC)理论的新颖应用来估算CNT悬浮液的电导率。仿真结果表明,流体的存在如何通过破坏CNT的低频声子来影响CNT传热的能力。 Irving-Kirkwood关系在空间上的使用揭示了局部热通量,阐明了复合材料中的传热路径。通过将CNT的集合体及其周围流体视为存在于液体中,可以将模型结果始终纳入HC理论。仿真结果表明理论与现有实验结果一致。

著录项

  • 来源
    《Journal of Heat Transfer》 |2015年第7期|072401.1-072401.8|共8页
  • 作者单位

    Department of Mechanical Engineering, Rice University, Houston, TX 77005;

    Department of Mechanical Engineering, Rice University, Houston, TX 77005;

    Department of Materials Science & Nanoengineering, Rice University, Houston, TX 77005;

    Thermal/Fluid Sciences & Engineering Department, Sandia National Laboratories, Livermore, CA 94550;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    heat transfer; nanofluids; carbon nanotubes; molecular dynamics;

    机译:传播热量;纳米流体碳纳米管;分子动力学;
  • 入库时间 2022-08-18 00:22:53

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