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

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Fate of Mercury in the Arctic 95<br />

Cx/Co = 0.82 exp ( - 22.53 (πDL/4Q)(d1+d2/d2-d1) (1)<br />

As seen from the equation, it is valid for collection efficiencies of 100% where the value of the<br />

mass concentration of the gas at a distance, Cx, over the mass concentration of the gas at the<br />

entrance, Co is less than 0.82. D is the diffusion coefficient of the gas in the air, and Q is the<br />

volumetric flow rate, d1 and d2 are the internal and external diameters of the annulus. Important<br />

assumptions for the above therefore are: 1., laminar flow must be obtained in the tube; 2., all the<br />

molecules reaching the wall must be trapped and should not diffuse chromatographically further<br />

into the tube; 3., The capacity of the trapping medium limits collection time, since eventually the<br />

active surface will become saturated and the gases will no longer be trapped on the wall, being<br />

carried through the denuder instead. This is what is known as breakthrough (Bemgård et al., 1996).<br />

These conditions must be satisfied for annular denuders to work as the RGM reservoir for the REA<br />

sampling system.<br />

Considering the results from the denuder tests, with the previously mentioned considerations<br />

and uncertainties, when sampling at 1 Hz, the above requirements are met. The denuders were<br />

simply not able to sample RGM at a sampling flow rate of 10 Hz. To do so, their geometry would<br />

need to be redesigned in accordance with the Gormley Kennedy equation. This would mean that<br />

they would need to be shorter and thicker. This would limit the development of laminar flow and is<br />

not rudimentary redesign work.<br />

One of the ideas for the future could then be to indirectly measure RGM using KCl coated<br />

beads in a quartz denuder tube, of the same dimension of the annular denuders in Landis et al., 2002<br />

and thereby facilitating, using the same analytical sampling chain and heating caps. This system<br />

would collect TPM + RGM. TPM could be measured alone with a co-located TPM collector and<br />

subtracted from the RGM+TPM, giving an indirect measurement of RGM. A TPM sampler could<br />

also be modified to collect RGM. This would take advantage of there being greater confidence in

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