The distribution of cloud-base mass flux is studied using large-eddy
simulations (LES) of two reference cases, one representing conditions over the
tropical ocean, and another one representing mid-latitude conditions over land.
To examine what sets the difference between the two distributions, nine
additional LES cases are set up as variations of the two reference cases. We
find that the total surface heat flux and its changes over the diurnal cycle do
not influence the distribution shape. The latter is also not determined by the
level of organization in the cloud field. It is instead determined by the ratio
of the surface sensible heat flux to the latent heat flux, the Bowen ratio B.
B sets the thermodynamic efficiency of the moist convective heat cycle, which
determines the portion of the total surface heat flux that can be transformed
into mechanical work of convection against mechanical dissipation. The
thermodynamic moist heat cycle sets the average mass flux per cloud ⟨m⟩, and through ⟨m⟩ it also controls the shape of the
distribution. An expression for ⟨m⟩ is derived based on the
moist convective heat cycle and is evaluated against LES. This expression can
be used in shallow cumulus parameterizations as a physical constraint on the
mass flux distribution. The similarity between the mass flux and the cloud area
distributions indicate that B also has a role in shaping the cloud area
distribution, which could explain its different shapes and slopes observed in
previous studies.Comment: submitted to J. Atmos. Sci., revise