  We show that one may pass from bulk to boundary thermodynamic quantities for
rotating AdS black holes in arbitrary dimensions so that if the bulk quantities
satisfy the first law of thermodynamics then so do the boundary CFT quantities.
This corrects recent claims that boundary CFT quantities satisfying the first
law may only be obtained using bulk quantities measured with respect to a
certain frame rotating at infinity, and which therefore do not satisfy the
first law. We show that the bulk black hole thermodynamic variables, or
equivalently therefore the boundary CFT variables, do not always satisfy a
Cardy-Verlinde type formula, but they do always satisfy an AdS-Bekenstein
bound. The universal validity of the Bekenstein bound is a consequence of the
more fundamental cosmic censorship bound, which we find to hold in all cases
examined. We also find that at fixed entropy, the temperature of a rotating
black hole is bounded above by that of a non-rotating black hole, in four and
five dimensions, but not in six or more dimensions. We find evidence for
universal upper bounds for the area of cosmological event horizons and
black-hole horizons in rotating black-hole spacetimes with a positive
cosmological constant.
