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Regimes of Rarefied Gas Flows

Part of the Fluid Mechanics and Its Applications book series (FMIA, volume 83)

Abstract

Consider the steady-state flow of an infinite stream of a rarefied gas over a body having a characteristic dimension, R, in the absence of external forces. In this case, the Boltzmann equation may be expressed in the form:
$$ v \cdot \frac{{\partial f}} {{\partial \tilde r}} = \iiint {\left( {f'f'_1 - ff_1 } \right)}gbdbd\varepsilon dv_1 . $$
(6-1)

Keywords

Boltzmann Equation Knudsen Number Accommodation Coefficient Knudsen Layer Tangential Momentum Accommodation Coefficient 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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