Multiplying successively the kinetic Eq. 2.11.14 with the collision integral (Eq. 2.11.20) by 1, components of n vector, components of the tensor n¡nk - (l/3)Sik, and integrating over the angular variables in the momentum space, we obtain a set of equations for the quantities n, j, dn T p d n p dn m
— + divl = u——— + divu—— + — dt 3 dpdr
3 _ . .[uhf I + m | u dp-I + — (iuhjl), (2.11.24)
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