|
Titel |
Air–snowpack exchange of bromine, ozone and mercury in the springtime Arctic simulated by the 1-D model PHANTAS – Part 2: Mercury and its speciation |
VerfasserIn |
K. Toyota, A. P. Dastoor, A. Ryzhkov |
Medientyp |
Artikel
|
Sprache |
Englisch
|
ISSN |
1680-7316
|
Digitales Dokument |
URL |
Erschienen |
In: Atmospheric Chemistry and Physics ; 14, no. 8 ; Nr. 14, no. 8 (2014-04-25), S.4135-4167 |
Datensatznummer |
250118638
|
Publikation (Nr.) |
copernicus.org/acp-14-4135-2014.pdf |
|
|
|
Zusammenfassung |
Atmospheric mercury depletion events (AMDEs) refer to a recurring depletion
of mercury occurring in the springtime Arctic (and Antarctic) boundary layer,
in general, concurrently with ozone depletion events (ODEs). To close some of
the knowledge gaps in the physical and chemical mechanisms of AMDEs and ODEs,
we have developed a one-dimensional model that simulates multiphase chemistry
and transport of trace constituents throughout porous snowpack and in the
overlying atmospheric boundary layer (ABL). This paper constitutes Part 2 of
the study, describing the mercury component of the model and its application
to the simulation of AMDEs. Building on model components reported in Part 1
("In-snow bromine activation and its impact on ozone"), we have developed a
chemical mechanism for the redox reactions of mercury in the gas and aqueous
phases with temperature dependent reaction rates and equilibrium constants
accounted for wherever possible. Thus the model allows us to study the
chemical and physical processes taking place during ODEs and AMDEs within a
single framework where two-way interactions between the snowpack and the
atmosphere are simulated in a detailed, process-oriented manner. Model runs
are conducted for meteorological and chemical conditions that represent the
springtime Arctic ABL characterized by the presence of "haze" (sulfate
aerosols) and the saline snowpack on sea ice. The oxidation of gaseous
elemental mercury (GEM) is initiated via reaction with Br-atom to form HgBr,
followed by competitions between its thermal decomposition and further
reactions to give thermally stable Hg(II) products. To shed light on
uncertain kinetics and mechanisms of this multi-step oxidation process, we
have tested different combinations of their rate constants based on published
laboratory and quantum mechanical studies. For some combinations of the rate
constants, the model simulates roughly linear relationships between the
gaseous mercury and ozone concentrations as observed during AMDEs/ODEs by
including the reaction HgBr + BrO and assuming its rate constant to be the
same as for the reaction HgBr + Br, while for other combinations the
results are more realistic by neglecting the reaction HgBr + BrO.
Speciation of gaseous oxidized mercury (GOM) changes significantly depending
on whether or not BrO is assumed to react with HgBr to form Hg(OBr)Br.
Similarly to ozone (reported in Part 1), GEM is depleted via bromine radical
chemistry more vigorously in the snowpack interstitial air than in the
ambient air. However, the impact of such in-snow sink of GEM is found to be
often masked by the re-emissions of GEM from the snow following the
photo-reduction of Hg(II) deposited from the atmosphere. GOM formed in the
ambient air is found to undergo fast "dry deposition" to the snowpack by
being trapped on the snow grains in the top ~1 mm layer. We
hypothesize that liquid-like layers on the surface of snow grains are
connected to create a network throughout the snowpack, thereby facilitating
the vertical diffusion of trace constituents trapped on the snow grains at
much greater rates than one would expect inside solid ice crystals.
Nonetheless, on the timescale of a week simulated in this study, the signal
of atmospheric deposition does not extend notably below the top 1 cm of the
snowpack. We propose and show that particulate-bound mercury (PBM) is
produced mainly as HgBr42− by taking up GOM into bromide-enriched
aerosols after ozone is significantly depleted in the air mass. In the
Arctic, "haze" aerosols may thus retain PBM in ozone-depleted air masses,
allowing the airborne transport of oxidized mercury from the area of its
production farther than in the form of GOM. Temperature dependence of
thermodynamic constants calculated in this study for Henry's law and
aqueous-phase halide complex formation of Hg(II) species is a critical factor
for this proposition, calling for experimental verification. The proposed
mechanism may explain observed changes in the GOM–PBM partitioning with
seasons, air temperature and the concurrent progress of ozone depletion in
the high Arctic. The net deposition of mercury to the surface snow is shown
to increase with the thickness of the turbulent ABL and to correspond well
with the column amount of BrO in the atmosphere. |
|
|
Teil von |
|
|
|
|
|
|