A semiclassical theory of small oscillations is developed for nuclei that are
subject to velocity-dependent forces in addition to the usual interatomic
forces. When the velocity-dependent forces are due to a strong magnetic field,
novel effects arise -- for example, the coupling of vibrational, rotational,
and translational modes. The theory is first developed using Newtonian
mechanics and we provide a simple quantification of the coupling between these
types of modes. We also discuss the mathematical structure of the problem,
which turns out to be a quadratic eigenvalue problem rather than a standard
eigenvalue problem. The theory is then re-derived using the Hamiltonian
formalism, which brings additional insight, including a close analogy to the
quantum-mechanical treatment of the problem. Finally, we provide numerical
examples for the H2, HT, and HCN molecules in a strong magnetic field