For a classical gas with constant cross-sections, all first- and second-order dissipative transport coefficients are computed for arbitrary mass, and the non-relativistic limit reproduces Grad's equations.
p´1qq p2q` 1q!! ż dKf 0kEn´2q k ` m2´E2 k ˘q “ 1 p2q` 1q!!eα ż dΩ d|k| p2πq3 exp ´ ´β a |k|2`m2 ¯´ |k|2`m2 ¯n´2q´1 2 |k|2q`2 . Substituting y
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Relativistic dissipative hydrodynamics for particles of arbitrary mass
For a classical gas with constant cross-sections, all first- and second-order dissipative transport coefficients are computed for arbitrary mass, and the non-relativistic limit reproduces Grad's equations.