  We show that for an anomalous fluid carrying dissipationless chiral magnetic
and/or vortical currents there is a frame in which a stationary obstacle
experiences no drag, but energy and charge currents do not vanish, resembling
superfluidity. However, unlike ordinary superfluid flow, the anomalous chiral
currents do transport entropy in this frame. We show that the second law of
thermodynamics completely determines the amounts of these anomalous
non-dissipative currents in the "no-drag frame" as polynomials in temperature
and chemical potential with known anomaly coefficients. These general results
are illustrated and confirmed by a calculation in the chiral kinetic theory and
quark-gluon plasma at high temperature.
