Samples of analyses

Figure 11: Event on June 18, 1997, 17:00 - 19:00 in Graz /
Austria

Figure 12: DSD for the most intense period of this event.
MP-DSD (yellow), JD-DSD (green) and JT-DSD (red) indicated.
The DSD for the most intense period of this event (6 minutes - from 17:54 till 18:00) is given in the above figure, clearly indicating drops of more than 7 mm in equivolmetric sphere diameter. This is a very important result, since many distrometers used so far stop classifying drops at 5.5 mm equivolumetric sphere diameter. That makes a great difference in practically all DSD dependent applications (weather radar and wave propagation, soil erosion studies etc.).
Figure 13a: Raindrop measured at 17:55:32.996, equ. sph.
diameter = 6.12 mm, precise correction method applied.
Figure 13b: Raindrop measured at 17:55:07.013, equ. sph.
diameter = 7.52 mm, precise correction method applied.

Figure 14: Horizontal copolar radar reflectivity ZH
derived from the rainrate only (black line) and from the full DSD
info obtained by the distrometer. The black line represents an
approximation formula, closely related to the Marshall-Palmer
[1948] DSD (yellow line in the following picture for 6 minutes
period). Parameters: elevation angle = 0°, temperature = 10°C,
drop shape = ROPEX.
Whenever the red line exceeds the black one, this usually indicates that there are more 'big' drops than proposed by Marshall-Palmer (MP-DSD). It is clearly seen that considerable deviations occur, as also stated by Figure 12. Our measurements from all around the world indicate that the behaviour of DSDs is climate dependent.

Figure 15: DSD for a twenty minutes period of tropical rain (measured
in Lae/Papua New Guinea), class width = 0.1 mm, uncalibrated data below 0.6
mm. Rainrate = 25.24 mm/hr. Exponential DSDs: N0 = 8000 (yellow),
1400 (red), 30000 (green) /m3mm.
Figure 16a: Front view to be corrected for distortion due
to horizontal motion.
Figure 16b: Front view corrected by approximation method.
Figure 16c: Front view corrected by precise method,
canting angle = 18.8°.
Further samples of canted raindrops:

Figure 17a

Figure 17b
Figure 17c
Figure 17d
Figure 17e