The intermolecular interaction energy in crystalline urea has been calculat
ed both from diffraction data and from the Hartree-Fock crystalline electro
n-density distribution, using a modified atom-atom approximation scheme. Th
e electrostatic part of this energy has been calculated from the atomic mul
tipole moments, obtained by adjustment of the multipole model to experiment
al X-ray and to theoretical Hartree-Fock structure amplitudes. To obtain th
e induction energy, multipole moments were calculated from structure amplit
udes for the crystalline electron density and from those that refer to the
electron density of a superposition of isolated molecules. This worked well
for the calculation of the interaction energy from Hartree-Fock data (6% d
ifference from the sublimation-energy value), but not for the interaction e
nergy from experimental data, where the moments of the superposition have t
o come from Hartree-Fock calculations: the two sets of multipole moments ar
e far too different. The uncertainty of the phases of the structure amplitu
des, combined with systematic errors in the theoretical data and noise in t
he experimental values, may account for the discrepancies. The nature of th
e different contributions to intermolecular interactions for urea is examin
ed.