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The effective thermal conductivity of ballistic-diffusive heat conduction in nanostructures with internal heat source

机译:具有内部热源的纳米结构中弹道扩散热传导的有效导热系数

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In nanostructures whose characteristic lengths are comparable to the phonon mean free path, the ballistic-diffusive heat conduction leads to the size effect, geometry dependence and anisotropy of the effective thermal conductivity. In the present work, we have studied the effective thermal conductivity of the ballistic-diffusive heat conduction in nanostructures (including nanofilms and nanowires) with internal heat source using Monte Carlo simulation and Boltzmann transport equation. It is found that the effective thermal conductivity of nanostructures with internal heat source is significantly lower than that with temperature difference, though it still increases with the increasing characteristic length. The models for the effective thermal conductivity and the temperature distribution of the cross-plane heat conduction in the nanofilms with internal heat source are directly derived from the phonon Boltzmann transport equation, and the comparisons with the Monte Carlo simulations well confirm their validities. As for the effective thermal conductivity of the in-plane nanofilms and nanowires with internal heat source, referring to the Matthiessen's rule, the models are in the form of k_(eff)/k_(bulk) = 1/(1 + αKn), with the parameter a obtained by the best fitting with the Monte Carlo simulations. Moreover, the diffusive heat conduction equation with the effective thermal conductivity can well characterize the temperature distributions in the in-plane nanofilms and long nanowires, while it fails in the short nanowires due to the influence of the axial constraints.
机译:在特征长度可与声子平均自由程相当的纳米结构中,弹道扩散热传导导致有效导热率的尺寸效应,几何形状依赖性和各向异性。在目前的工作中,我们使用蒙特卡罗模拟和玻尔兹曼输运方程研究了内部热源的纳米结构(包括纳米膜和纳米线)中弹道扩散热传导的有效导热系数。发现具有内部热源的纳米结构的有效导热率显着低于具有温度差的纳米结构,尽管其仍随着特征长度的增加而增加。直接从声子玻尔兹曼输运方程推导了具有内部热源的纳米膜中有效导热系数和跨平面热传导的温度分布模型,并且与蒙特卡洛模拟的比较很好地证实了它们的有效性。至于具有内部热源的面内纳米膜和纳米线的有效导热率,参考Matthiessen法则,模型的形式为k_(eff)/ k_(bulk)= 1 /(1 +αKn),参数a是通过蒙特卡罗模拟的最佳拟合获得的。此外,具有有效热导率的扩散导热方程可以很好地表征面内纳米膜和长纳米线中的温度分布,而在短纳米线中则由于轴向约束的影响而失效。

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