The shape of averaged drop size distributions (DSD) is studied from a
large sample of data (892 h) collected at several sites of various lat
itudes. The results show that neither the hypothesis of an exponential
distribution to represent rainfall with a high rain rate (R) nor the
concept of equilibrium distribution arising from the various models us
ing the parameterization of Low and List is compatible with the observ
ations. To describe the DSD two regions have to be distinguished: a sm
all-drop region, for diameter D smaller than a threshold D-c, and a la
rge-drop region, for diameter D larger than D-c. For D < D-c the distr
ibutions are strongly dependent on R and on z(0), the height of fall o
f the rain from the base of the melting level. The decrease in tile re
lative number of small drops with increasing R suggests that in this r
egion the depletion of the small drops by the big ones is not totally
compensated for by the input of small drops due to the collisional bre
akup process; there is no stationary state for D < D-c. In the big-dro
p region, for D > D-c, the slope of the distributions is almost indepe
ndent of D. At low values of R (<20 mm h(-1)) it decreases when R incr
eases, and not much depends on z(0). For increasing values of R beyond
about 20 mm h(-1), the slope of the distributions tends toward a cons
tant value of about 2.2-2.3 mm(-1). This suggests a certain stationari
ty between the coalescence and collisional breakup processes in intens
e rainfalls. It also appears that the two regions are not much influen
ced by each Ether. The value of D-c increases with R and with z(0). Th
e relation between the radar reflectivity factor (Z) and R obtained fr
om the averaged DSDs are close to those calculated from nonaveraged da
ta and compatible with those proposed in the literature. The differenc
es observed between the coefficients of Z-R relations for various type
s of rain are essentially due to the differences in small-drop concent
ration.