Abstract
For nonconvective, steady light rain with rain rates <5 mm h−1 the mean Doppler velocity of raindrop spectra was found to be constant below the melting band, when the drop-free fall speed was adjusted for pressure. The Doppler radar–weighted raindrop diameters varied from case to case from 1.5 to 2.5 mm while rain rates changed from 1.2 to 2.9 mm h−1. Significant changes of advected velocity moments were observed over periods of 4 min.
These findings were corroborated by three independent systems: a Doppler radar for establishing vertical air speed and mean terminal drop speeds [using extended Velocity Azimuth Display (EVAD) analyses], a Joss–Waldvogel disdrometer at the ground, and a Particle Measuring System (PMS) 2-DP probe flown on an aircraft. These measurements were supported by data from upper-air soundings. The reason why inferred raindrop spectra do not change with height is the negligible interaction rate between raindrops at low rain rates. At low rain rates, numerical box models of drop collisions strongly support this interpretation. It was found that increasing characteristic drop diameters are correlated with increasing rain rates.
* Current affiliation: Environment Canada, Pacific and Yukon Region, Meteorological Service of Canada, Vancouver Office, Vancouver, British Columbia, Canada
+ Current affiliation: Meteorological Service of Canada, King City, Ontario, Canada
# Current affiliation: Department of Atmospheric Sciences, University of Illinois at Urbana–Champaign, Urbana, Illinois
Corresponding author address: Dr. Robert Nissen, Environment Canada, Pacific and Yukon Region, Meteorological Service of Canada, 201–401 Burrard Street, Vancouver, BC V6C 3S5, Canada. Email: robert.nissen@ec.gc.ca
