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

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Fate of Mercury in the Arctic 105<br />

A more exact determination of the surface resistance was not possible with the available output<br />

data from the pilot REA system. However, the new NOAA system produces the necessary output<br />

factors to allow modeled calculation of ra and rm in accordance with the Karlsson and Nyholm dry<br />

deposition and desorption model (Karlsson and Nyholm, 1998); i.e., friction velocity, Obukov’s<br />

length and the stratification function as long as a diffusion coefficient for RGM is known. Therefore<br />

campaigns with the new system will provide a better approximation of depositional velocity and<br />

surface resistance.<br />

As seen in Figure 14., page 77, the depositional velocities noted for depositional events are<br />

fast, around 2 cm s -1 this is what would be expected for a very reactive gaseous species such as<br />

HNO3. On average, the depositional velocity is approximately 1 cm s -1 . Comparing with measured<br />

dry deposition velocities over snow for HNO3, reviewed in Karlson and Nyholm, 1998, show that<br />

the measured dry depositional velocities for RGM may be an order of magnitude higher than that<br />

for HNO3, given the snow surface temperature of < 2 0 C. However, there are also reported values<br />

that fall within the range found for RGM in this study. For example, Cress et al.,1995, as cited in<br />

Karlsson and Nyholm, found the depositional velocity about 0 0 C to be in the range of 0.88-3.79,<br />

though the air concentration is not given. It is seen that as ambient concentrations of HNO3<br />

decreased, depositional velocities apparently increased: for a concentration in the air of 6-15 µg m -3<br />

Johansson and Granath, 1986, find a depositional velocity for air temperatures < -2 0 C of HNO3 to<br />

be 0.02 – 0.1 cm s -1 ; near 0 0 C the deposition velocity increases, to 0.6 cm s -1 . Cadle et al., 1985,<br />

as cited in Karlsson and Nyholm, report a depositional velocity averaged for all temperatures, with<br />

an air concentration of 6 µg m -3 to be 1.4 cm s -1 .<br />

Comparing the depositional velocities found in this study with the experimental data reported<br />

for HNO3 shows that while the expected values could have been an order of magnitude lower, the

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