The hydrogen ͑H͒ solubility isotherms and the relative partial enthalpy-and entropy of H in a MoV / V͑001͒ superlattice in the range 0 ഛ ͓H/V͔ ഛ 1 ͓atomic ratio͔ are addressed. The difference in solubility between MoV and V assures that H only resides in the 22Å thick V layers, and the use of MoV instead of Mo increases the range of reversibility of the uptake, for the actual strain state. The biaxial elastic constraints, imposed by the H-free layers and the substrate, are shown to have a big influence on the H -H interaction. At low H content, the mean H -H interaction is close to zero, while for ͓H/V͔ 0.25, the interaction becomes attractive. We show that for a film constrained to expand in one dimension, the elastic dipole interaction is zero when the H-induced local strain field is isotropic, whereas for an anisotropic local strain field the interaction energy can be attractive, if the strain axes are parallel aligned with the direction of the expansion. Based on the symmetries of the respective local strain fields, we interpret the onset of the attractive H -H interaction at ͓H/V͔Ϸ0.25 as a self-induced change of H site occupancy, from tetrahedral to octahedral sites.