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FATE OF MERCURY IN THE ARCTIC Michael Evan ... - COGCI

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3.1 RGM flux measurements<br />

The results of the 2001 campaign in Alaska: Barrow Arctic Mercury Study (BAMS -2001) are<br />

shown in Table 1 and Fig. 1. The largest deposition velocity in 2001 was 2.7 cm s -1 and the average<br />

was close to 1 cm s -1 . Mean dry depositional flux was found to be - 0.4 ± 0.2 pg m -2 s -1 .<br />

Concentrations of the three denuder tubes, up, mid and down, were added together to determine the<br />

total concentration, and concentration was compared with the on site Tekran automatic RGM<br />

monitor, MODEL 1130, described in Lindberg et al., 2002 (Table 1).<br />

The machines were not running absolutely simultaneously so a linear interpretation was made<br />

to compare concentrations. Not taking run two into account, since a valve was frozen open, it is<br />

seen that the percent difference varies, with an average for the campaign of 24% with a standard<br />

deviation of 42%. The percent difference between the two measurements was between 3% and<br />

78%. This variance can be explained as a combination of the comparison method, the systems were<br />

not started or stopped simultaneously, and the oxidation of gaseous elemental mercury to RGM is<br />

dynamic, thus a linear extrapolation of concentration during a sampling period, is conservative. It is<br />

seen that in all but 2 of the runs, run 2 excluded, the RGM REA total is less than the TEKRAN<br />

1130 value, perhaps because of differences in the heating mantle system, but this observed bias<br />

could also be because of different flow calibration systems.<br />

The REA system when properly on the tower, after a period of time should report the same<br />

number of counts per up and down channel, due to conservation of mass, and did so when initially<br />

inventoried and tested during pre-deployment trials in Oak Ridge. In Barrow, there was always a<br />

greater number, up to 30% more, of counts on the down channel, suggesting that the sonic<br />

anemometer was not positioned properly, or a forcing of the turbulence. Therefore the channel<br />

count data was corrected to ensure mass conservation as follows:<br />

1) Corrected counts in Down = registered counts in Down - (registered counts in Down –<br />

corrected Down); where corrected counts in down = counts in up channel.<br />

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