The resonating-group method developed for nuclear collisions is used to obtain equations describing the collisions of slow atoms. On one hand, these equations correctly take into account the indistinguishability of electrons and scattering boundary conditions and therefore are free from the drawbacks of conventional equations in the adiabatic electronic basis. On the other hand, they retain the form of the latter equations and therefore are in agreement with the generally accepted picture of heavy-particle motion in the fields of adiabatic electronic potentials accompanied by nonadiabatic transitions. The general theory is illustrated by considering the interaction of two ground-state hydrogen atoms in the Heitler-London electronic basis.PACS number(s): 34.10.+x, 34.40.+n[6] JM= -, 'MH was taken for all internuclear distances. It is to be noted here that in [20], trying to reproduce experimental highly excited vibrational levels of H2 on the basis of the best Kolos-%olniewicz potential for the X'X+ state, the authors had to fit an effective value for the reduced mass and obtained a value very near to -, 'MH.But such a choice is incompatible with the Born-Oppenheimer picture where the nuclei are assumed to move in the fields of adiabatic electronic potentialseigenenergies of the electronic Hamiltonian for clamped nuclei to which the so-called adiabatic correction is added (see, e.g. , [13]). The reduced mass of the nuclei enters the set of coupled equations corresponding to this picture