Effect of Interfacial Roughness on Phonon Radiative Heat Conduction

[+] Author and Article Information
A. Majumdar

Department of Mechanical and Aerospace Engineering, Arizona State University, Tempe, AZ 85287

J. Heat Transfer 113(4), 797-805 (Nov 01, 1991) (9 pages) doi:10.1115/1.2911206 History: Received December 17, 1990; Revised February 19, 1991; Online May 23, 2008


The interface between a solid and a liquid or two dissimilar solids poses a resistance to heat transport by phonons, which are quanta of lattice vibrational energy. The classical theory explains that the resistance R arises due to a mismatch in acoustic impedances of the two media and predicts R to vary with temperature T as R ~ T−3 . Experiments with copper and liquid 3 He have shown that first, although RT3 is a constant below 0.1 K, its value is much less than that predicted by the classical theory. Second, at higher temperatures the resistance behaves as R ~ T−n where n > 3. This study explains these observations in the temperature range of 0.06 K−1 K and 3 He pressure range from zero atmospheres in liquid state to solid state, by including the effects of surface roughness and phonon attenuation in solids by electrons or dislocations. Roughness measurements have shown that solid surfaces have a fractal structure and are characterized by a fractal dimension D lying between 2 and 3 for a surface. Using the fractal characteristics, the thermal boundary resistance is shown to follow the relation RT3 ~ (1 + ηTβ )−1 where β is a function of the dimension D and η is a scaling constant. The predictions are in excellent agreement with the experimental observations, indicating that, in addition to other surface effects, the fractal surface structure could have a strong influence on thermal boundary resistance.

Copyright © 1991 by The American Society of Mechanical Engineers
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