There is a close analogy between the dynamics of electrons in a strong
magnetic field and the dynamics of quantized vortices in superfluids
and superconductors. In both systems an important part is played by a
term in the Lagrangian linear in velocity that corresponds to a Berry
phase in the quantum theory. This Berry phase can be calculated from t
he usual trial wave function for a vortex. This has important conseque
nces for quantum tunnelling of vortices, and leads unambiguously to th
e form of the Magnus force in a superconductor.