No. Renno et al., RADIATIVE-CONVECTIVE MODEL WITH AN EXPLICIT HYDROLOGIC-CYCLE .2. SENSITIVITY TO LARGE CHANGES IN SOLAR FORCING, JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 99(D8), 1994, pp. 17001-17020
The one-dimensional radiative-convective equilibrium model with an exp
licit hydrologic cycle introduced in part 1 is used to study the sensi
tivity of the model's atmosphere to large changes in the solar forcing
, when various cumulus convection parameterizations are used. As shown
by Simpson [1927], by Komabayasi [19671, and by Ingersoll [1969] when
the concentration of the absorbing gas in the atmosphere is temperatu
re dependent, equilibrium is impossible for values of the solar forcin
g larger than a critical value. This result is referred to as a runawa
y greenhouse. The cumulus convection parameterization schemes currentl
y in use in global climate models (GCMs) employ different assumptions
about moistening. This causes the critical solar forcing above which a
runaway greenhouse occurs to be very sensitive to the cumulus convect
ion scheme employed. Futhermore, using the microphysically based cumul
us convection scheme proposed by Emanuel [1991], we show that the sens
itivity of the equilibrium temperature to changes in the solar forcing
depends crucially on the microphysics of cumulus convection. For fixe
d cloud conditions, the critical solar forcing for a runaway greenhous
e to occur is between approximately 1.22 and 1.49 times the global mea
n value for the Earth, and for clear sky conditions, it is a few perce
nt lower. The runaway greenhouse in the experiments with the mass flux
schemes generally occurs more rapidly than in the experiments with th
e adjustment schemes. In addition, the inability of the hard convectiv
e adjustment scheme to produce an efficient vertical transport of mois
ture, together with the saturation requirement for convection to occur
, leads to the breakdown of the radiative-convective equilibria when o
ther processes axe not available to provide the necessary vertical tra
nsport of water vapor.