Ja. Zehnder, A comparison of convergence- and surface-flux-based convective parameterizations with applications to tropical cyclogenesis, J ATMOS SCI, 58(3), 2001, pp. 283-301
The evolutions of radially symmetric vortices and idealized easterly waves
are compared using three simple convective parameterization schemes. The pa
rameterizations are formulated for a model atmosphere consisting of three c
oupled, shallow, constant-density layers. The first was developed by Ooyama
and later refined by DeMaria and Pickle (the ODP scheme). Their scheme use
s horizontal convergence in the boundary layer to define a vertical mass fl
ux, along with a closure relation based on conservation of moist static ene
rgy that determines the vertical redistribution of mass. The second scheme
is a modification of the ODP scheme in that convection is allowed to stabil
ize the profile. A third scheme has the convective mass flux from the bound
ary layer determined by the assumption that convective up- and downdrafts k
eep the equivalent potential temperature of the boundary layer in near equi
librium (the BLQ scheme).
For vortices that are initially radially symmetric, the ODP scheme produces
a hurricane-like vortex, provided that the middle atmosphere is sufficient
ly moist. However, the intensification is slow unless an unrealistically we
ak density stratification is used. For the modified ODP scheme, the vortex
intensifies on a shorter timescale in an atmosphere with a realistic strati
fication, regardless of the midlevel moisture profile. After the intensific
ation, convective transport of air with high equivalent potential temperatu
re stabilizes the profile, and the vortex begins to decay. For the BLQ sche
me, the vortex will intensify, provided that the middle atmosphere is suffi
ciently moist and after the atmosphere has been conditioned for deep convec
tion by the shallow convection.
For the idealized easterly waves, the development between the schemes is qu
ite different. Only the BLQ scheme allows convection to condition the atmos
phere for further deep convection, which results in a developing disturbanc
e.