In this paper, we investigate, by three-dimensional hydrodynamical sim
ulations, the role that vertical convective motions play in providing
angular momentum transport in a Keplerian disk. We begin by deriving s
imple and general analytic constraints upon the correlated radial and
azimuthal velocity fluctuation tensor, critical to the direction of en
ergy and angular momentum transport. When azimuthal pressure gradients
are small, as is often the case for incompressible turbulence in a sh
earing disk, the constraints are particularly straightforward and stri
king: they imply there can be no net outward transport in a steady flo
w. (More precisely, any steady transport that is present must be due t
o the explicit forcing by azimuthal pressure gradients.) Furthermore,
numerical simulations show inward transport even in disks characterize
d by solid body rotation, which are quite far from axisymmetric. If th
e kinetic energy of rotational velocity fluctuations increases with ti
me because of coupling with the mean flow (as in an instability), the
relationship suggests (and our numerical simulations confirm) that in
a Keplerian disk the Reynolds stress is negative, i.e., that the angul
ar momentum and energy transport is inward. The analogous relationship
for shearing but nonrotating (Cartesian) flow displays the opposite s
ign for the fluctuation tensor, i.e., an increase in the ''streamwise'
' velocity fluctuations is associated with outward (from higher moment
um to smaller momentum) transport. Although Cartesian shear flows are
known to be extremely sensitive to disruption by nonlinear secondary i
nstabilities, hydrodynamical calculations presented here demonstrate t
hat Keplerian disk flows show no such inclination. We suggest that the
key to understanding this critical difference is the very different n
ature of the interaction between the mean flow and the transport in ea
ch system. We provide a physical interpretation of our findings in ter
ms of the role epicyclic oscillations play in mediating angular moment
um transport. We base our convection simulations upon a reproducible a
nalytic expression for the vertical profile of an unstable equilibrium
state in a stratified disk. The nonlinear evolution of the convective
cells is then followed after the initial profile is perturbed. Convec
tion can be sustained only if an ad hoc source of heating is added to
the disk midplane. The net transport associated with steady convection
is small and on average inward. A comparison between the volume-avera
ged Reynolds stress and the time rate of change of the azimuthal kinet
ic energy associated with fluctuations in the rotational velocity show
s remarkable agreement with our simple analytic predictions. Taken as
a whole, these results offer little hope that convection-or any other
form of incompressible hydrodynamic turbulence-is likely to be a signi
ficant source of angular momentum transport in nonmagnetic disks. Cohe
rent pressure forcing by, e.g., spiral density waves, remains a viable
option.