Wc. Malm et Ml. Pitchford, COMPARISON OF CALCULATED SULFATE SCATTERING EFFICIENCIES AS ESTIMATEDFROM SIZE-RESOLVED PARTICLE MEASUREMENTS AT 3 NATIONAL LOCATIONS, Atmospheric environment, 31(9), 1997, pp. 1315-1325
Size distributions and resulting optical properties of sulfur aerosols
were investigated at three national parks by a Davis Rotating-drum Un
iversal-size-cut Monitoring (DRUM) impactor. Sulfur size distribution
measurements for 88, 177, and 315 consecutive time periods were made a
t Grand Canyon National Park during January and February 1988, Meadvie
w, AZ during July, August, and September 1992, and at Shenandoah Natio
nal Park during summer, 1990, respectively. The DRUM impactor is desig
ned to collect aerosols with an aerodynamic diameter between 0.07 and
15.0 mu m in eight size ranges. Focused beam particle-induced X-ray em
ission (PIXE) analysis of the aerosol deposits produces a time history
of size-resolved elemental composition of varied temporal resolution.
As part of the quality assurance protocol, an interagency monitoring
of protected visual environments (IMPROVE) channel A sampler collectin
g 0-2.5 mu m diameter particles was operated simultaneously alongside
the DRUM sampler. During these sampling periods, the average sulfur ma
ss, interpreted as ammonium sulfate, is 0.49, 2.30, and 10.36 mu g m(-
3) at Grand Canyon, Meadview, and Shenandoah, respectively. The five d
rum stages were ''inverted'' using the Twomey (1975) scheme to give 48
6 size distributions, each made up of 72 discreet pairs of dC/dlog(D)
and diameter (D). From these distributions mass mean diameters (D-g),
geometric standard deviations (sigma(g)), and mass scattering efficien
cies (e(m)) were calculated. The geometric mass mean diameters in asce
nding order were 0.21 mu m at Meadview, 0.32 mu m at Grand Canyon, and
0.42 mu m at Shenandoah. The corresponding sigma(g)'s were 2.1, 2.3,
and 1.9. Mie theory mass scattering efficiencies calculated from dC/dl
og(D) distributions for the three locations were 2.05, 2.59, and 3.81
m(2) g(-1), respectively. At Shenandoah, mass scattering efficiencies
approached five but only when the mass median diameters were approxima
tely 0.4 mu m and sigma(g)'s were about 1.5. sigma(g)'s near 1.5 were
frequently measured at Shenandoah, rarely at Grand Canyon, and never d
uring the summer at Meadview. (C) 1997 Elsevier Science Ltd.