The Penn State/NCAR Mesoscale Model (MM5) is used to; simulate the-precipit
ation event that occurred during 1-2 May 1994 to the south of the Yangtze R
iver. In five experiments the Kain-Fritsch scheme is made use of for the su
bgrid-scale convective precipitation, but five different resolvable-scale m
icrophysical parameterization schemes are employed. They are the simple sup
er-saturation removal scheme, the warm rain scheme of Hsie et al. (1984), t
he simple ice scheme of Dudhia (1989), the complex mixed-phase scheme devel
oped by Reisner et al. (1993), and the GSFC microphysical scheme with graup
el. Our interest is how the various resolvable-scale schemes affect the dom
ain-averaged precipitation, the precipitation distribution, the sea level p
ressure, the cloud water and the cloud ice.
Through a series of experiments about a warm sector rainfall case, results
show that although the different resolvable-scale scheme is used, the diffe
rences of the precipitation characteristics among all five runs are not ver
y obvious. However, the precipitation is over-predicted and the strong meso
scale low is produced by the simple super-saturation removal Scheme. The wa
rm rain-scheme with the inclusion of condensation and evaporation under-pre
dicts the precipitation and allows the cloud water to reach the 300 hPa lev
el. The scheme of the addition of graupel increases the resolvable-scale pr
ecipitation by about 20%-30%. The inclusion of supercooled liquid water-in
the grid-scale scheme does not affect significantly the results.