R. Avissar et Yq. Liu, 3-DIMENSIONAL NUMERICAL STUDY OF SHALLOW CONVECTIVE CLOUDS AND PRECIPITATION INDUCED BY LAND-SURFACE FORCING, JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 101(D3), 1996, pp. 7499-7518
A state-of-the-art mesoscale atmospheric model was used to investigate
the three-dimensional structure and evolution of shallow convective c
louds and precipitation in heterogeneous and homogeneous domains. In g
eneral, the spatial distribution of clouds and precipitation is strong
ly affected by the landscape structure. When the domain is homogeneous
, they appear to be randomly distributed. However, when the landscape
structure triggers the formation of mesoscale circulations, they conce
ntrate in the originally dry part of the domain, creating a negative f
eedback which tends to eliminate the landscape discontinuities, and sp
atially homogenize the land water content. The land surface wetness he
terogeneity of the domain and the total amount of water vapor present
in the atmosphere (locally evapotranspired and/or advected) affect the
precipitation regime. In general, the upward motion of mesoscale circ
ulations generated by landscape heterogeneities is stronger than therm
al cells induced by turbulence. Furthermore, their ability to transpor
t moist, warm air to higher elevations increases the amount of water t
hat can be condensed and precipitated. The evolution of shallow convec
tive clouds and precipitation consists of a ''build-up phase'' during
which turbulence is predominant and responsible for the moistening of
the atmosphere. In heterogeneous domains, it is also responsible for t
he creation of horizontal pressure gradients leading to the generation
of mesoscale circulations. This phase occurs during the morning hours
. From about 1200 until 1600 LST, clouds develop and most of the preci
pitation is produced. This is the ''active phase.'' After 1600 LST, th
e horizontal thermal and pressure gradients, which fed the energy nece
ssary to create and sustain the mesoscale circulations, gradually disa
ppear. This is the ''dissipation phase.'' The differences and similari
ties obtained between three-dimensional and two-dimensional simulation
s were also studied. These simulations indicate that, unless the lands
cape presents a clear two-dimensional structure, the use of such a two
-dimensional model is not appropriate to simulate this type of clouds
and precipitation. Conversely, two-dimensional simulations can be conf
idently used, provided that the simulated domain presents a two-dimens
ional heterogeneity.