Rf. Pueschel et al., AEROSOL ABUNDANCES AND OPTICAL CHARACTERISTICS IN THE PACIFIC BASIN FREE TROPOSPHERE, Atmospheric environment, 28(5), 1994, pp. 951-960
During NASA's Global Backscatter Experiment (GLOBE) mission flights in
November 1989 and May 1990, a DC-8 research aircraft probed the Pacif
ic Basin free troposphere for about 90 flight hours in each month betw
een +72 and -62 degrees latitude, +130 and -120 degrees longitude, and
up to 39,000 feet pressure altitudes. Aerosols were sampled continuou
sly in situ by optical particle counters to measure concentration and
particle size, and during 48 10-min intervals during each mission by w
ire impactors for concentration, size, composition, phase and shape an
alyses. The optical particle counters cover a particle diameter range
between 0.3 and 20 mum; wire impactors extend the range down to 0.03 m
um. Results of particle number, size, shape, together with the assumpt
ion of a refractive index corresponding to (NH4)2SO4 to account for th
e prevalence of aerosol sulfur, were utilized in a Mie algorithm to ca
lculate aerosol extinction and backscatter for a range of wavelengths
(0.385 < lambda < 10.64 mum). Computations for 22 randomly selected si
ze distributions yield coefficients of extinction E0.525 = (2.03 +/- 1
.20) x 10(-4) km-1 and backscatter beta0.525 = (6.45 +/- 3.49) x 10(-6
) km-1 sr-1 in the visible, and E10.64 = (8.13 +/- 6.47) x 10(-6) km-1
and beta10.64 = (9.98 +/- 10.69) x 10(-8) km-1 sr-1 in the infra-red,
respectively. Large particles (D > 0.3 mum) contribute two-thirds to
the total extinction in the visible (lambda = 0.525 mum), and almost 1
00% in the infra-red (lambda = 10.64 mum). These results have been use
d to define an IR optical aerosol climatology of the Pacific Basin fre
e troposphere, from which it follows that the infra-red backscatter co
efficient at lambda = 9.25 mum wavelength fluctuates between 5.0 x 10(
-10) and 2.0 x 10(-7) km-1 sr-1 with a modal value 2.0 x 10(-8) km-1 s
r-1.