M. Maki et al., Characteristics of the raindrop size distribution in tropical continental squall lines observed in Darwin, Australia, J APPL MET, 40(8), 2001, pp. 1393-1412
Disdrometer data measured during the passage of tropical continental squall
lines in Darwin, Australia, are analyzed to study characteristics of raind
rop size distribution (DSD). Fifteen continental squall lines were selected
for the DSD analysis. An observed squall line was partitioned into three r
egions based on radar reflectivity pattern, namely, convective line, strati
form, and reflectivity trough. A convective line was further partitioned in
to the convective center, leading edge, and trailing edge using a threshold
rain rate of 20 mm h(-1). Statistics of modified gamma DSD parameters obta
ined by a least squares fitting method show distinct differences between th
e convective-center and the stratiform regions; the shape of DSD for the co
nvective center is convex upward, but it is more exponential for the strati
form region; the intercept parameter N-0 of the modified gamma function for
the convective center and the reflectivity trough tends to be larger than
that for the stratiform region, also. The observed drop size distributions
are normalized to remove the effect of differences in rainfall rate. Gamma
distributions then are least squares fitted to the normalized DSD data to s
how distinct differences between the convective-center and the stratiform r
egions; the characteristics of the trailing-edge and reflectivity-trough re
gions are equivalent to those of the convective center. DSD changes associa
ted with the rainwater content variations are calculated using the obtained
normalized gamma DSD function and the observed D-0-M relationship. The sim
ulation demonstrates that the stratiform region is characterized by a large
r drop spectrum (i.e., the maximum drop diameter and the median volume diam
eter are larger for the stratiform region than the convective center and th
e reflectivity trough for DSD with the same rainwater content). The Waldvog
el "N-0 jump'' is clearly shown, and the large drop spectrum for the strati
form region suggests the importance of the aggregation mechanism above the
melting level in the stratiform region. The difference in the DSD for the c
onvective-center and the stratiform regions causes systematic differences i
n Z-R relationships (Z = AR(b)). A larger value for coefficient A in the st
ratiform region is found, but values of A and b change case by case; an inv
erse relationship between A and b (A = 10(3.22) b (-6.25)) is found for rai
nfall in the convective-center and the trailing-edge regions.