The rovibrational kinetic energy for an arbitrary number of rigid molecules
is computed. The result has the same general form as the kinetic energy in
the molecular rovibrational Hamiltonian, although certain quantities are a
ugmented to account for the rotational energy of the monomers. No specific
choices of internal coordinates or body frame are made in order to accommod
ate the large variety of such conventions. However, special attention is pa
id to how key quantities transform when these conventions are changed. An e
xample system is analysed explicitly as an illustration of the formalism.