Air deflectors (Chimavir Air Services, Ltd., Israel) were installed on
an agricultural aircraft and tests were run to investigate: (1) the a
lteration in downwind residue results (drift) due to release height, (
2) the influence on droplet sizes conducted with a laser drop size ana
lyzer in a wind tunnel, and (3) the changes in airflow near the spray
boom as observed from wind tunnel tests. A turbine-powered monoplane w
ith air defectors was evaluated for spray drift losses and deposit cha
racteristics in a cotton field. Air-burden residue from application he
ights of 3.0, 4.6, and 6.1 m were investigated using high-volume air s
amplers along a 610-m sampler line oriented at 23.6-degrees from a 700
-m flightline. Spray deposit was measured (concurrent with the downwin
d airborne drift sampling) from collection of residue on Mylar plastic
sheets spaced at 61-m intervals from the first air sampler to beyond
the flightline. Gas chromatographic analysis was used to measure the c
oncentration of cinnamyl alcohol tracer. Results from air samplers ind
icated that the 3.0-m release height had significantly (P = 0.05) less
airborne drift (2.19 ppm) than the 4.6 m height (9.52 ppm) and 6.1 m
height (11.37 ppm). No differences (P = 0.05) in fallout deposit level
s were detected, although the 4.6 m height tended to have a higher lev
el of deposit (6.06 ppm) than the 3.0 m height (4.29 ppm) and the 6.1
m height (4.62 ppm). Spray droplet sizes produced in a wind tunnel wit
h and without a deflector were examined for a custom-sized RF 25-degre
es fan nozzle (3.06 L/min at 276 kPa, Delavan-Delta, Inc., Lexington,
Tenn.) and a D6-46 disk and core nozzle (Spraying Systems Co., Wheaton
, Ill.). Both nozzles were oriented 45-degrees down and back with airs
tream velocities of 60 and 75 m/s. Water-soluble formulations were exa
mined and included (1) cinnamyl alcohol, (2) bifenthrin, and (3) water
. Overall mean droplet sizes (Malvern) with the deflector were 235 mum
, whereas without the deflector they were 182 mum. The downwash of air
around the deflector was quantified in terms of mean, steady-state ai
r velocity and direction. Measurement points were selected on a two-di
mensional grid that ran longitudinally with the axis of the wind tunne
l. Air was deflected to an angle of 50-degrees from horizontal. A 54 m
ls airflow was decelerated to 40 mls behind the deflector.