3D ORIGAMI by Ikuko Mitsuoka

By Ikuko Mitsuoka

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22) it has to be assumed that the temperature profile is to a good approximation linear, and that there is perfect or at least very streng thermal coupling of the medium to the wall. 2. 15,19) it should be emphasized that pure isotropic scattering is not a regular but an exceptional case. f(X) is desired, it is necessary to know the temperature dependence of calorimetric and optical parameters. 15,19). 25 1. 7 Three Independent Methods to Determine Extinction Coefficients Experimental investigations that are reviewed in this volume comprise (calorimetric) measurements of thermal conductivities and optical experiments to detect extinction, absorption and scattering properties.

Recent experiments again illustrate large fluctuations in a [Themas 1967; Springer 1971; Saxena and Afshar 1985]. The werk of Saxena confirms the Undings of Roberts and Michels (see above) because an increase of a with increasing gas pressure is observed. The reader will intuitively follow Kostylev [1964] who assumes that several layers of adsorbed molecules on a disperse material at low temperatures are favourable to equalize thermal states of colliding molecules. Since adsorbed layers disappear at elevated temperatures, accommodation will decrease.

Contrary to the foregoing section we will now discuss methods to calculate expllcitly pure contact heat flow. Quantitative expressions that have been developed for our purpese regularly apply the thermal resistor model: the total thermal resistance Rs of a dispersed medium is calculated as the sum of a series of locally defined resistance uni ts. Each resistance uni t consists of four partial resistors that are switched partly in series, partly parallel. 5): one of the partial resistors (1) is defined with respect to the thermal conductivi ty of the solid material of which the particles are made.

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