Abstract:
It was shown in [1] that kernels $L_l(v,v_1)$ of linear collision integral and kernels $G^l_{l,0}(v, v_1, v_2)$ of nonlinear collision integral are related by the Laplace transform. Here, analytical expressions are derived for nonlinear kernels $G^{+l}_{l,0}(v, v_1, v_2)$ with arbitrary $l$ for models of hard spheres and pseudo-Maxwellian molecules using the Laplace transform method.