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A method is presented which, in principle, enables one to calculate higher-order coefficients for transport in fluids. To illustrate this theory the second-order terms in the pressure tensor which depend on the mass velocity are presented and evaluated approximately in terms of a microscopic relaxation time. Under certain approximations it is found that it is possible to sum the higher-order terms to every order.
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Storer et al. (1962) studied this question.
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