The equations governing a. collision of two slow multielectron atoms with n
onzero spins and orbital angular momentums in a finite electron basis are d
erived using the method of resonant groups. The equations take proper accou
nt of the identity of electrons, and the boundary conditions for scattering
and, therefore, are not subject to the well known drawbacks of the standar
d equations for scattering of atoms in the adiabatic electron basis. On the
other hand, the new equations have the same form as the equations of the c
onventional theory in the adiabatic basis and do not contradict the qualita
tive pattern of inelastic atomic collisions inferred from them. The express
ions derived for the matrix elements of nonadiabatic Coriolis interaction a
nd coupling between even and odd electron states for the case of isotope re
placement in a homonuclear system are unambiguous and depend only on the ch
oice of a finite electron basis.