FATE OF MERCURY IN THE ARCTIC Michael Evan ... - COGCI
FATE OF MERCURY IN THE ARCTIC Michael Evan ... - COGCI
FATE OF MERCURY IN THE ARCTIC Michael Evan ... - COGCI
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the literature of the reactions of Hg o with halogen atoms are also listed. All laboratory results are<br />
obtained using relative rate conditions.<br />
The reactions of halogens with Hg are independent of temperature (29,30) and therefore results of<br />
the various studies should be directly comparable. On the other hand ozone reactions with halogen<br />
atoms are temperature dependent and thus the rate constants obtained here of Hg are calculated at<br />
233 K and 263 K representative for the conditions in Arctic during mercury depletion.<br />
In general the half-life of GEM at Station Nord is 3 to 10 hours during an AMDE. Using rate<br />
constants of the latest study (31) this lifetime corresponds to a concentration of Br or Cl at 1-3 pptv<br />
and 0.1-0.3 pptv, respectively. Laboratories report Cl concentrations in the Arctic during AMDEs<br />
from 0.001 to 0.004 ppt (24,32,33), at least a factor of 25 lower in concentration than needed for the<br />
observed GEM depletion, whereas Br in the ppt level is reported by many authors (24,25,32,33).<br />
This implies that Br most probably is the key species leading to mercury depletion.<br />
Based on the results presented above the most important reactant for GEM removal is Br and the<br />
results in the study indicate a second order reaction rate constant of about 1•10 -12 cm 3 molec -1 sec -1 .<br />
The above result needs confirmation in the laboratory and though the result is a strong indication of<br />
the removal channel for GEM other possibilities needs to be examined before a definite answer can<br />
be given. In particular, it is important to clarify the role of heterogeneous chemistry during<br />
AMDE’s. Furthermore, there is a factor 16 difference in the reaction rate constant of the reaction<br />
between Br and Hg o reported (34,31) and in both cases determined by the relative rate technique.<br />
The difference shows that secondary reactions in the laboratory systems clearly plays a role and<br />
thus the reaction rate constant needs to be determined by an absolute method. To the knowledge of<br />
the authors there is not any study of the reaction rates constant of the reactions between Hg and ClO<br />
or BrO in the literature. Interesting enough there is good agreement between the theoretical<br />
calculated rate constant (27) and the rate constant extracted from the field measurements presented<br />
here. However, that might be a coincidence.<br />
The reaction between Br and Hg o leads to the formation of a radical.<br />
Hg + Br → HgBr •<br />
(9).<br />
The further fate of this radical is at the moment speculative but is the subject for a theoretical study<br />
(27,35).<br />
Modelling<br />
The mercury model has been run for October 1998 to October 2002 and the model results for GEM<br />
(Hg o ) are compared with measurements from Station Nord. The model does a good job reproducing<br />
the occurrence and length of AMDE but the simple parameterisation does not and cannot describe<br />
the fast variations in the period during the spring period, (Fig. 5). However, the main structure is<br />
reproduced and the results present a large step forward in the understanding of the fate of mercury<br />
in the Arctic atmosphere. The reproduction of the main structure is a strong indication for that the<br />
limiting factor is the surface conditions, which has to be sea ice with surface temperature below –4<br />
o C. A comparison of three model runs with observed GEM is shown in Fig. 5. The three model runs<br />
are: 1) without depletion, 2) with depletion where lifetime during depletion is 10 hours, and 3) with<br />
depletion and lifetime on 3 hours. The main difference between the two last runs with depletion is<br />
only a slightly higher minimum level in the case of 10 hour life time. The variations and duration of<br />
episodes are not changed.<br />
6