Re. Hillamo et al., DISTRIBUTIONS OF ATMOSPHERIC TRACE-ELEMENTS AT DYE-3, GREENLAND .1. DISTRIBUTION CHARACTERISTICS AND DRY DEPOSITION VELOCITIES, Atmospheric environment. Part A, General topics, 27(17-18), 1993, pp. 2787-2802
Cascade impactor samples were collected at Dye 3 on the south-central
Greenland Ice Sheet during March 1989. The impactor was calibrated in
the laboratory, and the resulting collection efficiency curves were us
ed to derive the impactor response for use in a data inversion procedu
re. The impactor samples were chemically analysed by proton-induced X-
ray emission (PIXE), and the chemical concentration data were used wit
h the inversion procedure to generate smooth size distributions for 15
elements. Results show three distinct size distribution categories. T
he first category includes elements that mainly originate from gas to
particle conversion, with a substantial fraction-from anthropogenic co
mbustion (S, Pb, Zn, Br and Ni). These elements exhibit a unimodal siz
e distribution with geometric mean aerodynamic diameter close to 0.6 m
u m, although S and in shaw a weak second mode centered at about 2 mu
m. Elements in the second category (Ti, Si, Fe, Mn, Ca, K) exhibit bim
odal size distributions, with geometric mean diameters for the two mod
es of 0.6 and 2 mu m, respectively. These elements result from a varie
ty of sources, including crustal erosion as well as combustion from na
tural and anthropopenic sources. For elements in the third category (A
l, Cl, Na, Mg), most of the mass occurs in particle sizes above 1 mu m
. Their size distribution is generally unimodal, with the geometric me
an aerodynamic diameter around 2 mu m. These elements are most likely
to be of crustal and/or marine origin. The best-fit size distributions
were used with curves of dry deposition velocity vs aerodynamic parti
cle diameter to estimate the overall dry deposition velocity expected
from the entire distribution. The deposition velocities for S, Pb, Zn,
Br and Ni are all very low, with values less than about 0.02 cm s(-1)
if hygroscopic growth in the humid layer is neglected. For those othe
r elements, deposition velocities are in the range 0.2-0.7 cm s(-1). F
or those distributions that are bimodal, the upper mode generally domi
nates deposition even when most of he airborne mass is associated with
the lower modes, as in the case of S and Zn.