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Effective thermal conductivity of disperse materials. Ⅱ. Effect of external load

机译:分散材料的有效导热率。 Ⅱ。外部负载的影响

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Using the steady-state heat flux method, the effective thermal conductivity X of a particle bed is measured at room temperature, varying the external load P on the bed in the range of 3-30 kPa. Grains of various forms (debris, pebble, cubo-octahedral) and balls of different materials (polypropylene, sodium chloride, ceramics, diamonds, metals) of which the thermal conductivity of the solid measures 0.2-1500 W/(m K) are used. From the experimental dependencies λ(P) = λ_0 + Δλ(P), values for effective thermal conductivity in the absence of contact heat conduction λ_0 and contact conductivity Δλ(P) are found. The analysis allowed us (a) to refine further our earlier evaluation (in the first part of this study Abyzov et al. (2013)) of the adequacy of models which do not take account of contact thermal conductivity (the differential effective medium model and those of Gusarov et al., Raghavan-Martin, Chiew-Glandt/Gonzo, Kunii et al., Zehner-Schlunder) and (b) to assess the capabilities provided by a number of models of contact thermal conductivity (those of Dul'nev-Sigalova, Kaganer, Gusarov and others). A model with nominally flat rough contacts between particles in the bed is proposed, which describes the observed effects for contact thermal conductivity.
机译:使用稳态热通量方法,在室温下测量颗粒床的有效热导率X,使颗粒床的外部负载P在3-30 kPa的范围内变化。使用各种形式的颗粒(碎屑,卵石,立方八面体)和不同材料的球(聚丙烯,氯化钠,陶瓷,钻石,金属),其中固体的导热系数为0.2-1500 W /(m K) 。从实验依赖性λ(P)=λ_0+Δλ(P),发现在没有接触热传导λ_0和接触热导率Δλ(P)的情况下有效热导率的值。通过分析,我们(a)可以进一步完善我们先前的评估(在本研究的第一部分,Abyzov等人(2013年)),其中没有考虑接触热导率的模型(差分有效介质模型和Gusarov等人,Raghavan-Martin,Chiew-Glandt / Gonzo,Kunii等人,Zehner-Schlunder的模型)和(b)评估由多种接触热导率模型提供的能力(Dul'nev的模型) -Sigalova,Kaganer,Gusarov等)。提出了在床中的颗粒之间具有名义上平坦的粗糙接触的模型,该模型描述了观察到的接触热导率的影响。

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