Thermal conductances in a collisionless gas between coaxial cylinders and concentric spheres

1967 ◽  
Vol 1 (2) ◽  
pp. 209-217 ◽  
Author(s):  
Yau Wu

The thermal conductances in a collisionless gas between coaxial cylinders and concentric spheres have been obtained for arbitrary thermal accommodation coefficients. This exact theory is based on the general theory of thermal conduction of collisionless gas developed recently by Wu which has been established according to his revised theory of thermal transpiration. The classical theory of thermal conductance between coaxial cylinders by Knudsen and Von Smoluchowski is only accurate to the first power of the temperature difference in which the velocity distribution in the system is assumed to be nearly Maxwellian. However, in the present paper, it is unnecessary to make this usual assumption and the exact theory has been established according to the revised theory of thermal transpiration.

2011 ◽  
Vol 82 (3) ◽  
pp. 035120 ◽  
Author(s):  
Wayne M. Trott ◽  
Jaime N. Castañeda ◽  
John R. Torczynski ◽  
Michael A. Gallis ◽  
Daniel J. Rader

Author(s):  
K. J. Daun ◽  
P. H. Mercier ◽  
G. J. Smallwood ◽  
F. Liu ◽  
Y. Le Page

Laser-induced incandescence (LII) is used to measure the thermal accommodation coefficient between soot sampled from a well-characterized flame and various monatomic and polyatomic gases. These measurements show that the thermal accommodation coefficient between soot and monatomic gases increases with molecular mass due to the decreasing speed of incident gas molecules and corresponding decrease in surface deformation rate, and that energy is transferred preferentially from the surface to the translational mode of the polyatomic gas molecules over internal energy modes.


2014 ◽  
Vol 136 (8) ◽  
Author(s):  
Toshiyuki Doi

Plane thermal transpiration of a rarefied gas between two walls of Maxwell-type boundaries with different accommodation coefficients is studied based on the linearized Boltzmann equation for a hard-sphere molecular gas. The Boltzmann equation is solved numerically using a finite difference method, in which the collision integral is evaluated by the numerical kernel method. The detailed numerical data, including the mass and heat flow rates of the gas, are provided over a wide range of the Knudsen number and the entire range of the accommodation coefficients. Unlike in the plane Poiseuille flow, the dependence of the mass flow rate on the accommodation coefficients shows different characteristics depending on the Knudsen number. When the Knudsen number is relatively large, the mass flow rate of the gas increases monotonically with the decrease in either of the accommodation coefficients like in Poiseuille flow. When the Knudsen number is small, in contrast, the mass flow rate does not vary monotonically but exhibits a minimum with the decrease in either of the accommodation coefficients. The mechanism of this phenomenon is discussed based on the flow field of the gas.


1967 ◽  
Vol 46 (6) ◽  
pp. 2376-2386 ◽  
Author(s):  
Frank O. Goodman ◽  
Harold Y. Wachman

2005 ◽  
Author(s):  
N. Mingo ◽  
D. A. Broido

Quantum upper bounds to thermal conductance are computed for zigzag single walled carbon nanotubes of different diameters. Upper bounds to energy and entropy flow are also computed. The results impose a stringent limit on the maximum values that any experiment or simulation could obtain. Some previous theoretical simulations have violated the theoretical maxima.


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