275practically completely explained in terms of modulations of the average structure which are of the £2 symmetry, even though the average crystal structure corresponds to a frozen-in £, modulation.We argue that the short-range order, which tends locally to preserve the c-glide plane, is due to dipoledipole interactions between molecules. On the other hand, the stability of the lattice over a long range (corresponding to wavevectors close to q = 0) is governed by the short-range repulsive interactions and the ability of the molecules to form a closely packed structure in three different crystallographic planes. In agreement with the general conclusions of Kitaigorodsky (1973) the BEMB2 molecules are more easily able to do this in the space group P21 than in Pc. The 'hole' represents a range of wavevectors for which the strain from the packing forces, as a result of the local breaking of the P21 symmetry, outweighs the energy gained from the short-range ordering of the molecular dipoles. sities, a partitioning of the calculated PE over contact types, the average PE per atom in the molecule, and the number of contacts per atom within a 7/k sphere. The molecular coordination number in hydrocarbon crystals is studied by partitioning the PE in successive shells of four to twelve neighbour molecules; the first (four-molecule) shell contributes 33 to 77% of PE, depending on various factors; the contribution of the twelve-molecule shell is invariably close to 100%.