The electronic contribution to the moment of inertia of single-channel
metal rings is analyzed. In rings threaded by a magnetic flux, the el
ectron moment I(e) exhibits a periodic pattern with maxima at PHI0=hc/
e or 1/2 PHI0 (modulo PHI0) depending on the number of electrons. For
slowly rotating rings, I(e) diverges in the limit of weak disorder. Th
e rotational anomalies rely on the same interference mechanism respons
ible for persistent currents and the Aharonov-Bohm effect.