Abstract
An investigation has been made of the time smoothing properties of the transport equations previously derived by the author [J. Chem. Phys. 26, 1421 (1957)]. A model is introduced, wherein momentum is transferred from one portion of a fluid medium to another via acoustical waves. This model is applied to the problem of viscous flow of a rare gas, and it is found that it is permissible and desirable to allow the time smoothing interval τ to become infinitely large. In practice this means that τ≫β—1, where β is a friction constant. The model incidentally yields a value for the viscosity coefficient in fair agreement with the Chapman‐Enskog hard sphere value.

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