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CONSTITUTIVE MODEL THEORIES AND ISSUES AND PLAUSIBLE PROPOSITIONS/CHALLENGES TO HEAT TRANSPORT CHARACTERIZATION

机译:本构模型理论与问题及诸如热传输表征的合理主张/挑战

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The present exposition describes the fundamental issues encompassing some prominent constitutive model theories governing macroscale/microscale heat conduction phenomenon with generalizations drawn concerning the physical relevance and the role of relaxation/retardation times including plausible propositions and challenges to heat transport characterization. Emanating from the Jeffreys type heat-flux constitutive model with physical interpretation provided as comprised of a linear combination of the Fourier and Cattaneo processes respectively, the consequences leading to the Cattaneo heat-flux model and subsequently the Fourier heat-flux model for both macroscale/microscale heat transport are addressed. For macroscale and microscale heat transport, the relevance to the notion of the so-called macroscale and microscale heat conduction model number is then drawn. As such, a generalized one-step [GOS] macroscale heat conduction formulation of the Jeffreys' type with consequences to the hyperbolic one-step [HOS] and the parabolic one-step [POS] formulations are particularly addressed. In addition, for microscale heat transport employing a two-temperature theory, the role of a microscale heat conduction model number is described via a generalized two-step [GTS] relaxation/retardation time-based heating model for use in specialized applications with consequences to the hyperbolic and parabolic two-step HTS/PTS and the HOS/POS formulations respectively. Efforts to provide plausible characterization of the microscale heat conduction model number are undertaken for microscale heat conduction applications by comparisons to available experiments as related to sudden short laser pulse heating of thin films including identifying potential challenges. We define the macroscale/microscale heat conduction model number, F{sub}T and F{sub}(T{sub}e), respectively as: F{sub}T ≌ (Fourier Conductivity(k{sub}F))/(Fourier Conductivity(k{sub}F)+Cattaneo Conductivity(k{sub}C)) F{sub}(T{sub}e) ≌ (Electron Fourier Conductivity(k{sub}(e{sub}F)))/(Electron Fourier Conductivity(k{sub}(e{sub}F))+Electron Cattaneo Conductivity(k{sub}(e{sub}C))) Several noteworthy issues on heat conduction constitutive models are also highlighted. The pros/cons and limitations and a variety of deficiencies existing to date are also described and some of the conceptual pitfalls and issues encompass: (i) Pitfalls in attempting to explain microscale heat transport effects via macroscale heat conduction formulations. (ii) The issues of bounds for macroscale and microscale heat conduction. (iii) On pseudo time dimensional quantities. (iv) The pitfalls of dropping higher-order time derivative terms in the microscale heat transport equations under order-of-magnitude arguments. (v) On a conditional alias of the Jeffreys' type heat flux model provided underlying physics is not being violated.
机译:本博览会描述涵盖与管理有关的物理意义和松弛/延迟时间,包括合理的命题,并以热传输表征挑战方面的作用得出的概括宏观/微观热传导现象的一些著名的本构模型理论的基本问题。从与物理解释的杰弗里型热通量构模型提供作为包含在傅立叶的线性组合的和郭居静分别处理,发出导致两个宏观的郭居静热通量模型,随后将傅立叶热通量模型的后果/微型热传输得到解决。对于宏观和微观热传输,是否适用于所谓的宏观和微观热传导型号的概念,然后绘制。因此,广义一步法[GOS]宏观热传导杰弗里斯类型的与后果双曲线一步法[HOS]和抛物线一步法制剂[POS]制剂是特别处理。此外,对于采用两温度理论微尺度热输送,微尺度热传导模型数的作用,是通过广义两步描述GTS]使用松弛/相位差基于时间的加热模型与后果专门的应用程序双曲线和抛物线两步HTS / PTS和分别居屋/ POS制剂。努力以提供微尺度导热模型号码的似是而非的表征是通过比较进行了微尺度热传导应用程序可用的实验作为与薄膜包括识别潜在挑战的突然短激光脉冲加热。我们定义宏观尺度/微米尺度的热传导模型号,F {子} t与t'{子}(T {子} e)中,分别为:F {子}Ť≌(傅立叶导率(K {子} F))/ (傅立叶导率(K {子} F)+郭居静导率(K {子} C))的F {子}(T {子} E)≌(电子傅立叶导率(K {子}(E {子} F)) )/(电子傅立叶导率(K {子}(E {}子F))+电子郭居静导率(K {子}(E {}子C)))上的热传导构模型的几个显着的问题也突出显示。在试图解释通过宏观热传导制剂微尺度热传输效果(ⅰ)缺陷:所述优点/缺点和局限性和各种现有的最新缺陷还描述和一些概念缺陷和问题的涵盖。 (ⅱ)边界为宏观和微观的热传导的问题。 (三)关于伪时间维的数量。 (iv)根据命令的数量级参数中的微型热传递方程滴高阶时间导数项的缺陷。 (ⅴ)在所提供的杰弗里型热通量模型的条件别名基本物理不被违反。

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