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

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Fate of Mercury in the Arctic 72<br />

and the additive product of the denuders, up, mid, down were within 25% of the constantly sampled<br />

denuder. There was a good mass balance between the up and down channel.<br />

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

shown in Table 1. page 73 and Figure 14 page 77. The largest deposition velocity in 2001 was<br />

approximately 2.8 cm s -1 and the average was close to 1 cm s -1 . Concentrations of the three denuder<br />

tubes, up, mid and down, were added together to determine the total concentration, and<br />

concentration was compared with the on site Tekran automatic RGM monitor, MODEL 1130,<br />

described in Lindberg et al., 2002, Appendix C. Since the machines were not running absolutely<br />

simultaneously, a linear interpretation was made to compare concentrations for the same time<br />

frame. The heating system for the annular denuder heating system for the 1130 kept the denuders<br />

warmer than the heating mantles on the REA system. Not taking run two into account, since a<br />

valve was frozen open, it is seen that the percent difference varies, with an average for the<br />

campaign of 24% with a standard deviation of 42. Percent difference between the two<br />

measurements was as small as 3% and as large as 78%. It is seen that in all but 2 of the runs, run 2<br />

excluded, the RGM REA total is less than the 1130 value, perhaps because of differences in the<br />

heating mantle system or in differences of flow calibration between the two 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 prior to<br />

deployment in Barrow at Walker Branch. In Barrow, there was always a greater number, up to 30%<br />

more, of counts on the down channel, suggesting that the sonic anemometer was not positioned<br />

properly. Therefore the channel count data was corrected to ensure mass conservation as follows:<br />

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

Control: total counts for all channels registered = total counts with down corrected.<br />

2) Corrected Counts for Mid = registered Counts for Mid - (Registered Counts for Down - corrected<br />

counts for Down); The lost mass must be placed in mid channel for later concentration calculation.<br />

Control: Corrected counts Mid > registered counts mid, but total counts all channels still the same.<br />

3) Corrected Counts Up = Old Counts up Up, since down was preferred during sampling.

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