We derive coupled, equations of motion for the condensate (superfluid)
and noncondensate (normal fluid) degrees of freedom in a trapped Bose
gas at finite temperatures. Our results are based on the Hartree-Fock
-Popov approximation for the time-dependent condensate wave function,
and thermodynamic local equilibrium for the noncondensate atoms. In th
e special case of a uniform weakly interacting gas, our hydrodynamic e
quations are shown to be consistent with the two-fluid equations of La
ndau. The collective modes in a parabolically trapped Bose gas include
the analog of the out-of-phase second-sound mode in superfluid He-4.