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Modeling the Atmospheric Transport
and Deposition of Mercury
Materials assembled for
“Mercury in Maryland” Meeting, Appalachian Lab,
Univ. of Maryland Center for Environmental Science
301 Braddock Road, Frostburg MD, Nov 2-3, 2005
Dr. Mark Cohen
NOAAAir Resources Laboratory
1315 East West Highway,
R/ARL, Room 3316
Silver Spring, Maryland, 20910
301-713-0295 x122;
mark.cohen@noaa.gov
http://www.arl.noaa.gov/ss/transport/cohen.html
1. Atmospheric
mercury
modeling
3. What do
atmospheric
mercury models
need?
2. Why do we
need
atmospheric
mercury
models?
4. Some
preliminary
results:
 Model evaluation
 Source Receptor
Information
2
1. Atmospheric
mercury
modeling
3. What do
atmospheric
mercury models
need?
2. Why do we
need
atmospheric
mercury
models?
4. Some
preliminary
results:
 Model evaluation
 Source Receptor
Information
3
CLOUD DROPLET
cloud
Primary
Anthropogenic
Emissions
Hg(II), ionic mercury, RGM
Elemental Mercury [Hg(0)]
Particulate Mercury [Hg(p)]
Re-emission of previously
deposited anthropogenic
and natural mercury
Hg(II) reduced to Hg(0)
by SO2 and sunlight
Hg(0) oxidized to dissolved
Hg(II) species by O3, OH,
HOCl, OCl-
Adsorption/
desorption
of Hg(II) to
/from soot
Natural
emissions
Upper atmospheric
halogen-mediated
heterogeneous oxidation?
Polar sunrise
“mercury depletion events”
Br
Dry deposition
Wet deposition
Hg(p)
Vapor phase:
Hg(0) oxidized to RGM
and Hg(p) by O3, H202,
Cl2, OH, HCl
Multi-media interface
Atmospheric Mercury Fate Processes
4
NOAA HYSPLIT MODEL
5
6
1. Atmospheric
mercury
modeling
3. What do
atmospheric
mercury models
need?
2. Why do we
need
atmospheric
mercury
models?
4. Some
preliminary
results:
 Model evaluation
 Source Receptor
Information
7
Why do we need atmospheric mercury models?
 to get comprehensive source attribution information ---
we don’t just want to know how much is depositing at any
given location, we also want to know where it came from…
 to estimate deposition over large regions,
…because deposition fields are highly spatially variable,
and one can’t measure everywhere all the time…
 to estimate dry deposition
 to evaluate potential consequences of alternative future
emissions scenarios
But models
must have
measurements Modeling
needed to help
interpret
measurements
and estimate
source-receptor
relationships
Monitoring
required to
develop models
and to evaluate
their accuracy
1. Atmospheric
mercury
modeling
3. What do
atmospheric
mercury models
need?
2. Why do we
need
atmospheric
mercury
models?
4. Some
preliminary
results:
 Model evaluation
 Source Receptor
Information
10
Emissions
Inventories
Meteorological
Data
Scientific understanding of
phase partitioning,
atmospheric chemistry,
and deposition processes
Ambient data for comprehensive
model evaluation and improvement
What do atmospheric
mercury models need?
11
some challenges facing mercury modeling
emissions
inventories
• need all sources
• accurately divided into different Hg forms
• U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005
• temporal variations (e.g. shut downs)
meteorological
data
• precipitation not well characterized
scientific
understanding
• what is RGM? what is Hg(p)?
• accurate info for known reactions?
• do we know all significant reactions?
• natural emissions, re-emissions?
ambient data for
model evaluation
• Mercury Deposition Network (MDN) is great, but:
• also need RGM, Hg(p), and Hg(0) concentrations
• also need data above the surface (e.g., from aircraft)
• also need source-impacted sites (not just background)
12
0 - 15 15 - 30 30 - 60 60 - 120 120 - 250
distance range from source (km)
0.001
0.01
0.1
1
10
100
hypothetical
1
kg/day
source
deposition
flux
(ug/m2-yr)
for
Hg(II) emit
Hg(p) emit
Hg(0) emit
Logarithmic
Why is emissions speciation information critical?
13
Hypothesized rapid reduction of Hg(II) in plumes?
If true, then dramatic impact on modeling results…
some challenges facing mercury modeling
emissions
inventories
• need all sources
• accurately divided into different Hg forms
• U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005
• temporal variations (e.g. shut downs)
meteorological
data
• precipitation not well characterized
scientific
understanding
• what is RGM? what is Hg(p)?
• accurate info for known reactions?
• do we know all significant reactions?
• natural emissions, re-emissions?
ambient data for
model evaluation
• Mercury Deposition Network (MDN) is great, but:
• also need RGM, Hg(p), and Hg(0) concentrations
• also need data above the surface (e.g., from aircraft)
• also need source-impacted sites (not just background)
14
some challenges facing mercury modeling
emissions
inventories
• need all sources
• accurately divided into different Hg forms
• U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005
• temporal variations (e.g. shut downs)
meteorological
data
• precipitation not well characterized
scientific
understanding
• what is RGM? what is Hg(p)?
• accurate info for known reactions?
• do we know all significant reactions?
• natural emissions, re-emissions?
ambient data for
model evaluation
• Mercury Deposition Network (MDN) is great, but:
• also need RGM, Hg(p), and Hg(0) concentrations
• also need data above the surface (e.g., from aircraft)
• also need source-impacted sites (not just background)
15
Reaction Rate Units Reference
GAS PHASE REACTIONS
Hg0 + O3  Hg(p) 3.0E-20 cm3/molec-sec Hall (1995)
Hg0 + HCl  HgCl2 1.0E-19 cm3/molec-sec Hall and Bloom (1993)
Hg0 + H2O2  Hg(p) 8.5E-19 cm3/molec-sec Tokos et al. (1998) (upper limit based
on experiments)
Hg0 + Cl2  HgCl2 4.0E-18 cm3/molec-sec Calhoun and Prestbo (2001)
Hg0 +OHC  Hg(p) 8.7E-14 cm3/molec-sec Sommar et al. (2001)
AQUEOUS PHASE REACTIONS
Hg0 + O3  Hg+2 4.7E+7 (molar-sec)-1 Munthe (1992)
Hg0 + OHC  Hg+2 2.0E+9 (molar-sec)-1 Lin and Pehkonen(1997)
HgSO3  Hg0 T*e((31.971*T)-12595.0)/T) sec-1
[T = temperature (K)]
Van Loon et al. (2002)
Hg(II) + HO2C  Hg0 ~ 0 (molar-sec)-1 Gardfeldt & Jonnson (2003)
Hg0 + HOCl  Hg+2 2.1E+6 (molar-sec)-1 Lin and Pehkonen(1998)
Hg0 + OCl-1  Hg+2 2.0E+6 (molar-sec)-1 Lin and Pehkonen(1998)
Hg(II)  Hg(II) (soot) 9.0E+2 liters/gram;
t = 1/hour
eqlbrm: Seigneur et al. (1998)
rate: Bullock & Brehme (2002).
Hg+2 + h<  Hg0 6.0E-7 (sec)-1 (maximum) Xiao et al. (1994);
Bullock and Brehme (2002)
Atmospheric Chemical Reaction Scheme for Mercury
1
some challenges facing mercury modeling
emissions
inventories
• need all sources
• accurately divided into different Hg forms
• U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005
• temporal variations (e.g. shut downs)
meteorological
data
• precipitation not well characterized
scientific
understanding
• what is RGM? what is Hg(p)?
• accurate info for known reactions?
• do we know all significant reactions?
• natural emissions, re-emissions?
ambient data for
model evaluation
• Mercury Deposition Network (MDN) is great, but:
• also need RGM, Hg(p), and Hg(0) concentrations
• also need data above the surface (e.g., from aircraft)
• also need source-impacted sites (not just background)
17
Some Additional Measurement Issues
(from a modeler’s perspective)
• Data availability
• Simple vs. Complex Measurements
Some Additional Measurement Issues
(from a modeler’s perspective)
• Data availability
• Simple vs. Complex Measurements
Data availability
A major impediment to evaluating and
improving atmospheric Hg models has been
the lack of speciated Hg air concentration data
There have been very few measurements to
date, and these data are rarely made available
in a practical way (timely, complete, etc.)
The data being collected at Piney
Reservoir could be extremely helpful!
Some Additional Measurement Issues
(from a modeler’s perspective)
• Data availability
• Simple vs. Complex Measurements
wet dep
monitor
Simple vs. Complex Measurements:
1. Wet deposition is a very complicated phenomena...
 many ways to get the “wrong” answer –
incorrect emissions, incorrect transport,
incorrect chemistry, incorrect 3-D precipitation,
incorrect wet-deposition algorithms, etc..
ambient air
monitor
models need ambient air concentrations
first, and then if they can get those right,
they can try to do wet deposition...
?
?
?
monitor
at ground
level
Simple vs. Complex Measurements:
2. Potential complication with ground-level monitors...
(“fumigation”, “filtration”, etc.)...
monitor above
the canopy
 atmospheric phenomena are complex and not well understood;
 models need “simple” measurements for diagnostic evaluations;
 ground-level data for rapidly depositing substances (e.g., RGM) hard to interpret
 elevated platforms might be more useful (at present level of understanding)
?
Simple vs. Complex measurements - 3. Urban areas:
a. Emissions inventory poorly known
b. Meteorology very complex (flow around buildings)
c. So, measurements in urban areas not particularly useful
for current large-scale model evaluations
• Sampling near intense sources?
• Must get the fine-scale met “perfect”
Ok, if one wants
to develop
hypotheses
regarding
whether or not
this is actually a
source of the
pollutant (and
you can’t do a
stack test for
some reason!).
Sampling site?
Simple vs. Complex Measurements –
4: extreme near-field measurements
Complex vs. Simple Measurements –
5: Need some source impacted measurements
• Major questions regarding plume chemistry
and near-field impacts (are there “hot spots”?)
• Most monitoring sites are designed to be
“regional background” sites (e.g., most
Mercury Deposition Network sites).
• We need some source-impacted sites as well to
help resolve near-field questions
• But not too close – maybe 20-30 km is ideal (?)
1. Atmospheric
mercury
modeling
3. What do
atmospheric
mercury models
need?
2. Why do we
need
atmospheric
mercury
models?
4. Some
preliminary
results:
 Model evaluation
 Source Receptor
Information
27
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
28
Participants
D. Syrakov …………………………….. Bulgaria….NIMH
A. Dastoor, D. Davignon ……………… Canada...... MSC-Can
J. Christensen …………………………. Denmark…NERI
G. Petersen, R. Ebinghaus …………...... Germany…GKSS
J. Pacyna ………………………………. Norway…..NILU
J. Munthe, I. Wängberg ……………….. Sweden….. IVL
R. Bullock ………………………………USA………EPA
M. Cohen, R. Artz, R. Draxler ………… USA………NOAA
C. Seigneur, K. Lohman ………………..USA……... AER/EPRI
A. Ryaboshapko, I. Ilyin, O.Travnikov…EMEP……MSC-E
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
29
Intercomparison Conducted in 3
Stages
I. Comparison of chemical schemes
for a cloud environment
II. Air Concentrations in Short Term
Episodes
III. Long-Term Deposition and
Source-Receptor Budgets
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
30
Model Acronym Model Name and Institution Stage
I II III
CAM Chemistry of Atmos. Mercury model, Environmental Institute, Sweden
MCM Mercury Chemistry Model, Atmos. & Environmental Research, USA
CMAQ Community Multi-Scale Air Quality model, US EPA
ADOM Acid Deposition and Oxidants Model, GKSS Research Center, Germany
MSCE-HM MSC-E heavy metal regional model, EMEP MSC-E
GRAHM Global/Regional Atmospheric Heavy Metal model, Environment Canada
EMAP Eulerian Model for Air Pollution, Bulgarian Meteo-service
DEHM Danish Eulerian Hemispheric Model, National Environmental Institute
HYSPLIT Hybrid Single Particle Lagrangian Integrated Trajectory model, US NOAA
MSCE-HM-Hem MSC-E heavy metal hemispheric model, EMEP MSC-E
Participating Models
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
31
Anthropogenic Mercury Emissions Inventory
and Monitoring Sites for Phase II
(note: only showing largest emitting grid cells)
Mace Head, Ireland
grassland shore Rorvik, Sweden
forested shore
Aspvreten, Sweden
forested shore
Zingst, Germany
sandy shore
Neuglobsow, Germany
forested area
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
32
Total Gaseous Mercury (ng/m3) at Neuglobsow: June 26 – July 6, 1995
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 MEASURED
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 MSCE
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 CMAQ
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 GRAHM
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 EMAP
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 DEHM
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 ADOM
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 HYSPLIT
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
33
Total Particulate Mercury (pg/m3) at Neuglobsow, Nov 1-14,
1999
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
MEASURED
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
CMAQ
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
GRAHM
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
EMAP
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
DEHM
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
ADOM
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
HYSPLIT
02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov
0
50
100
150
MSCE
34
MSCE Neuglobsow RGM
0
10
20
30
40
50
60
11/1/1999
11/2/1999
11/3/1999
11/4/1999
11/5/1999
11/6/1999
11/7/1999
11/8/1999
11/9/1999
11/10/1999
11/11/1999
11/12/1999
11/13/1999
11/14/1999
Date
pg/m
3
Obs
Calc
a
CMAQ Neuglobsow RGM
0
10
20
30
40
50
60
70
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
pg/m
3
Obs
Calc
ADOM Neuglobsow RGM
0
10
20
30
40
50
60
70
11/1/99
11/2/99
11/3/99
11/4/99
11/5/99
11/6/99
11/7/99
11/8/99
11/9/99
11/10/99
11/11/99
11/12/99
11/13/99
11/14/99
Date
pg/m
3
Obs
Calc
a
EMAP Neuglobsow RGM
0
5
10
15
20
25
11/1/1999
11/2/1999
11/3/1999
11/4/1999
11/5/1999
11/6/1999
11/7/1999
11/8/1999
11/9/1999
11/10/1999
11/11/1999
11/12/1999
11/13/1999
11/14/1999
Date
pg/m
3
Obs
Calc
a
GRAHM Neuglobsow RGM
0
35
70
105
140
11/1/99
11/2/99
11/3/99
11/4/99
11/5/99
11/6/99
11/7/99
11/8/99
11/9/99
11/10/99
11/11/99
11/12/99
11/13/99
11/14/99
Date
pg/m
3
Obs
Calc
a
HYSPLIT Neuglobsow RGM
0
10
20
30
40
50
60
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
/99
pg/m
3
Obs
Calc
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Budgets
Dry Dep
Wet Dep
RGM
Hg(p)
Hg0
Chemistry
Conclu-
sions
Stage III
Stage II
Stage I
Intro-
duction
DEHM Neuglobsow RGM
0
6
12
18
24
30
11/1/1999
11/2/1999
11/3/1999
11/4/1999
11/5/1999
11/6/1999
11/7/1999
11/8/1999
11/9/1999
11/10/1999
11/11/1999
11/12/1999
11/13/1999
11/14/1999
Date
pg/m
3
Obs
Calc
a
Reactive Gaseous Mercury at
Neuglobsow, Nov 1-14, 1999
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
35
DE01 DE09 NL91 NO99 SE02 SE11 SE12 SE05 FI96
Monitoring Station
0.0
0.5
1.0
1.5
2.0
2.5
3.0
wet
Hg
deposition
(g/km2-month)
Obs
MSCE-HM
MSCE-HM-Hem
HYSPLIT
DEHM
EMAP
CMAQ
August 1999 Mercury Wet Deposition
1. Atmospheric
mercury
modeling
3. What do
atmospheric
mercury models
need?
2. Why do we
need
atmospheric
mercury
models?
4. Some
preliminary
results:
 Model evaluation
 Source Receptor
Information
36
Example of
Detailed Results:
1999 Results for
Chesapeake Bay
37
Geographical Distribution
of 1999 Direct Deposition
Contributions to the Chesapeake
Bay (entire domain)
38
Geographical Distribution of 1999 Direct Deposition
Contributions to the Chesapeake Bay (regional close-up)
39
Geographical Distribution of 1999
Direct Deposition Contributions to
the Chesapeake Bay (local close-up)
40
Largest Regional Individual Sources Contributing to
1999 Mercury Deposition Directly to the Chesapeake Bay
41
Largest Local Individual Sources Contributing to
1999 Mercury Deposition Directly to the Chesapeake Bay
42
Emissions and Direct Deposition Contributions from Different
Distance Ranges Away From the Chesapeake Bay
0 - 100
100 - 200
200 - 400
400 - 700
700 - 1000
1000 - 1500
1500 - 2000
2000 - 2500
> 2500
Distance Range from Chesapeake Bay (km)
0
20
40
60
80
Emissions
(metric
tons/year)
0
2
4
6
8
Deposition
Flux
(ug/m2-year)
Emissions
Deposition Flux
43
Top 25 Contributors to 1999 Hg Deposition Directly to the Chesapeake Bay
PhoenixServices
BrandonShores
StericycleInc.
Morgantown
ChalkPoint
NASAIncinerator
H.A.Wagner
NorfolkNavyYard
Hampton/NASAIncin.
ChesapeakeEnergyCtr.
Chesterfield
Yorktown
INDIAN RIVER
Roxboro
BALTIMORERESCO
Mt. Storm
Homer City
Keystone
BMWNC
PossumPoint
Montour
PhoenixServices
Belews Creek
Harrisburg Incin.
HarfordCo. Incin.
MD
MD
MD
MD
MD
VA
MD
VA
VA
VA
VA
VA
DE
NC
MD
WV
PA
PA
NC
VA
PA
MD
NC
PA
MD
0% 20% 40% 60% 80% 100%
Cumulative Fraction of Hg Deposition
0
5
10
15
20
25
Rank
coal-fired elec gen
other fuel combustion
waste incineration
metallurgical
manufacturing/other
44
Preliminary Results
for other Maryland
Receptors
45
Maryland Receptors Included in Recent Preliminary HYSPLIT-Hg
modeling (but modeling was not optimized for these receptors!)
46
Largest Modeled Atmospheric Deposition Contributors Directly to
Deep Creek Lake based on 1999 USEPA Emissions Inventory
(national view)
47
Largest Modeled Atmospheric Deposition Contributors Directly to
Deep Creek Lake based on 1999 USEPA Emissions Inventory
(regional view)
48
Largest Modeled Atmospheric Deposition Contributors Directly to
Deep Creek Lake based on 1999 USEPA Emissions Inventory
(close-up view)
49
Some Next Steps
Expand model domain to include global sources
Additional model evaluation exercises ... more sites, more time periods,
more variables
Sensitivity analyses and examination of atmospheric Hg chemistry
(e.g. marine boundary layer, upper atmosphere)
Simulate natural emissions and re-emissions of previously deposited Hg
Use more highly resolved meteorological data grids
Dynamic linkage with ecosystem cycling models
50
Conclusions
At present, many model uncertainties & data limitations
Models needed for source-receptor and other info
Monitoring data required to evaluate and improve models
For this, simple may be better than complex measurements
Some useful model results appear to be emerging
Future is much brighter because of this coordination!
51
Thanks
52
EXTRA
SLIDES
53
• Hg is present at extremely trace levels in the atmosphere
• Hg won’t affect meteorology (can simulate meteorology
independently, and provide results to drive model)
• Most species that complex or react with Hg are generally
present at much higher concentrations than Hg
• Other species (e.g. OH) generally react with many other compounds
than Hg, so while present in trace quantities, their concentrations cannot
be strongly influenced by Hg
•The current “consensus” chemical mechanism (equilibrium +
reactions) does not contain any equations that are not 1st order in Hg
• Wet and dry deposition processes are generally 1st order
with respect to Hg
Why might the atmospheric fate of mercury
emissions be essentially linearly independent?
54
Spatial interpolation
RECEPTOR
Impacts from
Sources 1-3
are Explicitly
Modeled
2
1
3
Impact of source 4 estimated from
weighted average of
impacts of nearby
explicitly modeled sources
4
55
• Perform separate simulations at each location for emissions
of pure Hg(0), Hg(II) and Hg(p)
[after emission, simulate transformations between Hg forms]
• Impact of emissions mixture taken as a linear combination
of impacts of pure component runs on any given receptor
56
“Chemical Interpolation”
Source
RECEPTOR
Impact of Source
Emitting
30% Hg(0)
50% Hg(II)
20% Hg(p)
=
Impact of Source Emitting Pure Hg(0)
0.3 x
Impact of Source Emitting Pure Hg(II)
0.5 x
Impact of Source Emitting Pure Hg(p)
0.2 x
+
+
57
58
Standard Source Locations in Maryland region during recent simulation
59
0 50 100 150 200 250 300 350
day of year
0
10
20
30
40
50
60
70
80
90
100
ug/m2-year
if
daily
dep
continuted
at
same
rate
daily value
weekly average
Illustrative example of total deposition at a location
~40 km "downwind" of a 1 kg/day RGM source
60
Eulerian grid
models give
grid-averaged
estimates –
…difficult to
compare against
measurement at a
single location
Geographic Distribution of Largest Anthropogenic Mercury
Emissions Sources in the U.S. (1999) and Canada (2000)
62
63
• In principle, we need do this for each source
in the inventory
• But, since there are more than 100,000
sources in the U.S. and Canadian inventory,
we need shortcuts…
• Shortcuts described in Cohen et al
Environmental Research 95(3), 247-265, 2004
64
Cohen, M., Artz, R., Draxler, R., Miller, P., Poissant, L.,
Niemi, D., Ratte, D., Deslauriers, M., Duval, R.,
Laurin, R., Slotnick, J., Nettesheim, T., McDonald, J.
“Modeling the Atmospheric Transport and Deposition of
Mercury to the Great Lakes.” Environmental Research
95(3), 247-265, 2004.
Note: Volume 95(3) is a Special Issue: "An Ecosystem Approach to
Health Effects of Mercury in the St. Lawrence Great Lakes", edited by
David O. Carpenter.
65
• For each run, simulate fate and transport everywhere,
but only keep track of impacts on each selected receptor
(e.g., Great Lakes, Chesapeake Bay, etc.)
• Only run model for a limited number (~100) of hypothetical,
individual unit-emissions sources throughout the domain
• Use spatial interpolation to estimate impacts from sources at
locations not explicitly modeled
66
0.1o x 0.1o
subgrid
for
near-field
analysis
source
location
67
0.1o x 0.1o
subgrid
for
near-field
analysis
source
location
68
69
70
71
72
0 - 15 15 - 30 30 - 60 60 - 120 120 - 250
distance range from source (km)
0.001
0.01
0.1
1
10
100
deposition
flux
(ug/m2-yr)
Hg(II) emit, 50 m
Hg(II) emit, 250 m
Hg(II) emit, 500 m
Hg(p) emit; 250 m
Hg(0) emit, 250 m
Source at Lat = 42.5, Long = -97.5; simulation for entire year 1996 using archived NGM meteorological data
Deposition flux within different distance ranges from a hypothetical 1 kg/day source
Hypothesized rapid reduction of Hg(II) in plumes?
If true, then dramatic impact on modeling results…
0 - 15 15 - 30 30 - 60 60 - 120 120 - 250
distance range from source (km)
0
10
20
30
40
hypothetical
1
kg/day
source
deposition
flux
(ug/m2-yr)
for
Hg(II) emit
Hg(p) emit
Hg(0) emit
Linear
Why is emissions speciation information critical?
74
Why is emissions speciation information critical?
0 - 15 15 - 30 30 - 60 60 - 120 120 - 250
distance range from source (km)
0
10
20
30
40
hypothetical
1
kg/day
source
deposition
flux
(ug/m2-yr)
for
Hg(II) emit
Hg(p) emit
Hg(0) emit
Linear
Logarithmic
0 - 15 15 - 30 30 - 60 60 - 120 120 - 250
distance range from source (km)
0.001
0.01
0.1
1
10
100
hypothetical
1
kg/day
source
deposition
flux
(ug/m2-yr)
for
Hg(II) emit
Hg(p) emit
Hg(0) emit
75
 The form of mercury emissions (elemental, ionic,
particulate) is often very poorly known,
but is a dominant factor in estimating deposition
(and associated source-receptor relationships)
 Questions regarding atmospheric chemistry of
mercury may also be very significant
 The above may contribute more to the overall
uncertainties in atmospheric mercury models than
uncertainties in dry and wet deposition algorithms
Emissions and Chemistry
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
77
Neuglobsow
Zingst
Aspvreten
Rorvik
Mace Head
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
78
Total Gaseous Mercury at Neuglobsow: June 26 – July 6,
1995
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 08-Jul
0.0
1.0
2.0
3.0
4.0
Total
Gaseous
Mercury
(ng/m3)
MEASURED
NW
NW
NW
N
N
S
SE
NW
Neuglobsow
EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury
Intro-
duction
Stage I Stage II Stage III Conclu-
sions
Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets
79
Total Gaseous Mercury (ng/m3) at Neuglobsow: June 26 – July 6, 1995
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 MEASURED
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 MSCE
Using default
emissions inventory
The emissions
inventory is a
critical input to
the models…
26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul
0
1
2
3
4 MSCE - UBA
Using alternative
emissions inventory
Some Additional Measurement Issues
(from a modeler’s perspective)
• Data availability
• Simple vs. Complex Measurements
• Process Information
Process Information:
1. Dry Deposition - Resistance Formulation
1
Vd = --------------------------------- + Vg
Ra + Rb + Rc + RaRbVg
in which
• Ra = aerodynamic resistance to mass transfer;
• Rb = resistance of the quasi-laminar sublayer;
• Rc = overall resistance of the canopy/surface (zero for particles)
• Vg = the gravitational settling velocity (zero for gases).
Dry Deposition
 depends intimately on vapor/particle partitioning and particle
size distribution information
 resistance formulation [Ra, Rb, Rc...]
 for gases, key uncertainty often Rc (e.g., “reactivity factor” f0)
 for particles, key uncertainty often Rb
 How to evaluate algorithms when phenomena hard to measure?
Atmosphere above the quasi-laminar sublayer
Quasi-
laminar
Sublayer
(~ 1 mm
thick)
Surface
Rb
Rc
Ra
Very small
particles can
diffuse through the
layer like a gas
Very large particles
can just fall
through the layer
In-between
particles can’t
diffuse or fall
easily so they
have a harder
time getting
across the layer
Wind speed = 0 (?)
Particle dry deposition phenomena
0.0001 0.001 0.01 0.1 1 10 100
particle diameter (microns)
1E-5
0.0001
0.001
0.01
0.1
1
Deposition
Velocity
(m/sec)
Rb assumed small ( = 10 sec/m) Slinn and Slinn
Typical Deposition Velocities Over Water with Different Rb Formulations
Diffusion high;
Vd governed by Ra
Diffusion low;
Settling velocity low;
Vd governed by Rb
Vd =
settling
velocity
Process information needed:
1. For particle dry deposition, must
have particle size distributions!
LAKE
ATMOSPHERE
Pollutant on
Suspended
Sediment
Pollutant
Truly
Dissolved
in Water
PROCESS
INFORMATION:
2. The gas-exchange
flux at a water
surface depends on
the concentration of
pollutant in the gas-
phase and the truly-
dissolved phase
(but these are rarely
measured…)
Gas-Phase
Pollutant
Particle-Phase
Pollutant

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Atmospheric Mercury Modeling Needs

  • 1. Modeling the Atmospheric Transport and Deposition of Mercury Materials assembled for “Mercury in Maryland” Meeting, Appalachian Lab, Univ. of Maryland Center for Environmental Science 301 Braddock Road, Frostburg MD, Nov 2-3, 2005 Dr. Mark Cohen NOAAAir Resources Laboratory 1315 East West Highway, R/ARL, Room 3316 Silver Spring, Maryland, 20910 301-713-0295 x122; mark.cohen@noaa.gov http://www.arl.noaa.gov/ss/transport/cohen.html
  • 2. 1. Atmospheric mercury modeling 3. What do atmospheric mercury models need? 2. Why do we need atmospheric mercury models? 4. Some preliminary results:  Model evaluation  Source Receptor Information 2
  • 3. 1. Atmospheric mercury modeling 3. What do atmospheric mercury models need? 2. Why do we need atmospheric mercury models? 4. Some preliminary results:  Model evaluation  Source Receptor Information 3
  • 4. CLOUD DROPLET cloud Primary Anthropogenic Emissions Hg(II), ionic mercury, RGM Elemental Mercury [Hg(0)] Particulate Mercury [Hg(p)] Re-emission of previously deposited anthropogenic and natural mercury Hg(II) reduced to Hg(0) by SO2 and sunlight Hg(0) oxidized to dissolved Hg(II) species by O3, OH, HOCl, OCl- Adsorption/ desorption of Hg(II) to /from soot Natural emissions Upper atmospheric halogen-mediated heterogeneous oxidation? Polar sunrise “mercury depletion events” Br Dry deposition Wet deposition Hg(p) Vapor phase: Hg(0) oxidized to RGM and Hg(p) by O3, H202, Cl2, OH, HCl Multi-media interface Atmospheric Mercury Fate Processes 4
  • 6. 6
  • 7. 1. Atmospheric mercury modeling 3. What do atmospheric mercury models need? 2. Why do we need atmospheric mercury models? 4. Some preliminary results:  Model evaluation  Source Receptor Information 7
  • 8. Why do we need atmospheric mercury models?  to get comprehensive source attribution information --- we don’t just want to know how much is depositing at any given location, we also want to know where it came from…  to estimate deposition over large regions, …because deposition fields are highly spatially variable, and one can’t measure everywhere all the time…  to estimate dry deposition  to evaluate potential consequences of alternative future emissions scenarios
  • 9. But models must have measurements Modeling needed to help interpret measurements and estimate source-receptor relationships Monitoring required to develop models and to evaluate their accuracy
  • 10. 1. Atmospheric mercury modeling 3. What do atmospheric mercury models need? 2. Why do we need atmospheric mercury models? 4. Some preliminary results:  Model evaluation  Source Receptor Information 10
  • 11. Emissions Inventories Meteorological Data Scientific understanding of phase partitioning, atmospheric chemistry, and deposition processes Ambient data for comprehensive model evaluation and improvement What do atmospheric mercury models need? 11
  • 12. some challenges facing mercury modeling emissions inventories • need all sources • accurately divided into different Hg forms • U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005 • temporal variations (e.g. shut downs) meteorological data • precipitation not well characterized scientific understanding • what is RGM? what is Hg(p)? • accurate info for known reactions? • do we know all significant reactions? • natural emissions, re-emissions? ambient data for model evaluation • Mercury Deposition Network (MDN) is great, but: • also need RGM, Hg(p), and Hg(0) concentrations • also need data above the surface (e.g., from aircraft) • also need source-impacted sites (not just background) 12
  • 13. 0 - 15 15 - 30 30 - 60 60 - 120 120 - 250 distance range from source (km) 0.001 0.01 0.1 1 10 100 hypothetical 1 kg/day source deposition flux (ug/m2-yr) for Hg(II) emit Hg(p) emit Hg(0) emit Logarithmic Why is emissions speciation information critical? 13 Hypothesized rapid reduction of Hg(II) in plumes? If true, then dramatic impact on modeling results…
  • 14. some challenges facing mercury modeling emissions inventories • need all sources • accurately divided into different Hg forms • U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005 • temporal variations (e.g. shut downs) meteorological data • precipitation not well characterized scientific understanding • what is RGM? what is Hg(p)? • accurate info for known reactions? • do we know all significant reactions? • natural emissions, re-emissions? ambient data for model evaluation • Mercury Deposition Network (MDN) is great, but: • also need RGM, Hg(p), and Hg(0) concentrations • also need data above the surface (e.g., from aircraft) • also need source-impacted sites (not just background) 14
  • 15. some challenges facing mercury modeling emissions inventories • need all sources • accurately divided into different Hg forms • U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005 • temporal variations (e.g. shut downs) meteorological data • precipitation not well characterized scientific understanding • what is RGM? what is Hg(p)? • accurate info for known reactions? • do we know all significant reactions? • natural emissions, re-emissions? ambient data for model evaluation • Mercury Deposition Network (MDN) is great, but: • also need RGM, Hg(p), and Hg(0) concentrations • also need data above the surface (e.g., from aircraft) • also need source-impacted sites (not just background) 15
  • 16. Reaction Rate Units Reference GAS PHASE REACTIONS Hg0 + O3  Hg(p) 3.0E-20 cm3/molec-sec Hall (1995) Hg0 + HCl  HgCl2 1.0E-19 cm3/molec-sec Hall and Bloom (1993) Hg0 + H2O2  Hg(p) 8.5E-19 cm3/molec-sec Tokos et al. (1998) (upper limit based on experiments) Hg0 + Cl2  HgCl2 4.0E-18 cm3/molec-sec Calhoun and Prestbo (2001) Hg0 +OHC  Hg(p) 8.7E-14 cm3/molec-sec Sommar et al. (2001) AQUEOUS PHASE REACTIONS Hg0 + O3  Hg+2 4.7E+7 (molar-sec)-1 Munthe (1992) Hg0 + OHC  Hg+2 2.0E+9 (molar-sec)-1 Lin and Pehkonen(1997) HgSO3  Hg0 T*e((31.971*T)-12595.0)/T) sec-1 [T = temperature (K)] Van Loon et al. (2002) Hg(II) + HO2C  Hg0 ~ 0 (molar-sec)-1 Gardfeldt & Jonnson (2003) Hg0 + HOCl  Hg+2 2.1E+6 (molar-sec)-1 Lin and Pehkonen(1998) Hg0 + OCl-1  Hg+2 2.0E+6 (molar-sec)-1 Lin and Pehkonen(1998) Hg(II)  Hg(II) (soot) 9.0E+2 liters/gram; t = 1/hour eqlbrm: Seigneur et al. (1998) rate: Bullock & Brehme (2002). Hg+2 + h<  Hg0 6.0E-7 (sec)-1 (maximum) Xiao et al. (1994); Bullock and Brehme (2002) Atmospheric Chemical Reaction Scheme for Mercury 1
  • 17. some challenges facing mercury modeling emissions inventories • need all sources • accurately divided into different Hg forms • U.S. 1996, 1999, 2003 / CAN 1995, 2000, 2005 • temporal variations (e.g. shut downs) meteorological data • precipitation not well characterized scientific understanding • what is RGM? what is Hg(p)? • accurate info for known reactions? • do we know all significant reactions? • natural emissions, re-emissions? ambient data for model evaluation • Mercury Deposition Network (MDN) is great, but: • also need RGM, Hg(p), and Hg(0) concentrations • also need data above the surface (e.g., from aircraft) • also need source-impacted sites (not just background) 17
  • 18. Some Additional Measurement Issues (from a modeler’s perspective) • Data availability • Simple vs. Complex Measurements
  • 19. Some Additional Measurement Issues (from a modeler’s perspective) • Data availability • Simple vs. Complex Measurements
  • 20. Data availability A major impediment to evaluating and improving atmospheric Hg models has been the lack of speciated Hg air concentration data There have been very few measurements to date, and these data are rarely made available in a practical way (timely, complete, etc.) The data being collected at Piney Reservoir could be extremely helpful!
  • 21. Some Additional Measurement Issues (from a modeler’s perspective) • Data availability • Simple vs. Complex Measurements
  • 22. wet dep monitor Simple vs. Complex Measurements: 1. Wet deposition is a very complicated phenomena...  many ways to get the “wrong” answer – incorrect emissions, incorrect transport, incorrect chemistry, incorrect 3-D precipitation, incorrect wet-deposition algorithms, etc.. ambient air monitor models need ambient air concentrations first, and then if they can get those right, they can try to do wet deposition... ? ? ?
  • 23. monitor at ground level Simple vs. Complex Measurements: 2. Potential complication with ground-level monitors... (“fumigation”, “filtration”, etc.)... monitor above the canopy  atmospheric phenomena are complex and not well understood;  models need “simple” measurements for diagnostic evaluations;  ground-level data for rapidly depositing substances (e.g., RGM) hard to interpret  elevated platforms might be more useful (at present level of understanding) ?
  • 24. Simple vs. Complex measurements - 3. Urban areas: a. Emissions inventory poorly known b. Meteorology very complex (flow around buildings) c. So, measurements in urban areas not particularly useful for current large-scale model evaluations
  • 25. • Sampling near intense sources? • Must get the fine-scale met “perfect” Ok, if one wants to develop hypotheses regarding whether or not this is actually a source of the pollutant (and you can’t do a stack test for some reason!). Sampling site? Simple vs. Complex Measurements – 4: extreme near-field measurements
  • 26. Complex vs. Simple Measurements – 5: Need some source impacted measurements • Major questions regarding plume chemistry and near-field impacts (are there “hot spots”?) • Most monitoring sites are designed to be “regional background” sites (e.g., most Mercury Deposition Network sites). • We need some source-impacted sites as well to help resolve near-field questions • But not too close – maybe 20-30 km is ideal (?)
  • 27. 1. Atmospheric mercury modeling 3. What do atmospheric mercury models need? 2. Why do we need atmospheric mercury models? 4. Some preliminary results:  Model evaluation  Source Receptor Information 27
  • 28. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 28 Participants D. Syrakov …………………………….. Bulgaria….NIMH A. Dastoor, D. Davignon ……………… Canada...... MSC-Can J. Christensen …………………………. Denmark…NERI G. Petersen, R. Ebinghaus …………...... Germany…GKSS J. Pacyna ………………………………. Norway…..NILU J. Munthe, I. Wängberg ……………….. Sweden….. IVL R. Bullock ………………………………USA………EPA M. Cohen, R. Artz, R. Draxler ………… USA………NOAA C. Seigneur, K. Lohman ………………..USA……... AER/EPRI A. Ryaboshapko, I. Ilyin, O.Travnikov…EMEP……MSC-E
  • 29. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 29 Intercomparison Conducted in 3 Stages I. Comparison of chemical schemes for a cloud environment II. Air Concentrations in Short Term Episodes III. Long-Term Deposition and Source-Receptor Budgets
  • 30. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 30 Model Acronym Model Name and Institution Stage I II III CAM Chemistry of Atmos. Mercury model, Environmental Institute, Sweden MCM Mercury Chemistry Model, Atmos. & Environmental Research, USA CMAQ Community Multi-Scale Air Quality model, US EPA ADOM Acid Deposition and Oxidants Model, GKSS Research Center, Germany MSCE-HM MSC-E heavy metal regional model, EMEP MSC-E GRAHM Global/Regional Atmospheric Heavy Metal model, Environment Canada EMAP Eulerian Model for Air Pollution, Bulgarian Meteo-service DEHM Danish Eulerian Hemispheric Model, National Environmental Institute HYSPLIT Hybrid Single Particle Lagrangian Integrated Trajectory model, US NOAA MSCE-HM-Hem MSC-E heavy metal hemispheric model, EMEP MSC-E Participating Models
  • 31. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 31 Anthropogenic Mercury Emissions Inventory and Monitoring Sites for Phase II (note: only showing largest emitting grid cells) Mace Head, Ireland grassland shore Rorvik, Sweden forested shore Aspvreten, Sweden forested shore Zingst, Germany sandy shore Neuglobsow, Germany forested area
  • 32. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 32 Total Gaseous Mercury (ng/m3) at Neuglobsow: June 26 – July 6, 1995 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 MEASURED 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 MSCE 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 CMAQ 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 GRAHM 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 EMAP 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 DEHM 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 ADOM 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 HYSPLIT
  • 33. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 33 Total Particulate Mercury (pg/m3) at Neuglobsow, Nov 1-14, 1999 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 MEASURED 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 CMAQ 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 GRAHM 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 EMAP 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 DEHM 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 ADOM 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 HYSPLIT 02-Nov 04-Nov 06-Nov 08-Nov 10-Nov 12-Nov 14-Nov 16-Nov 0 50 100 150 MSCE
  • 34. 34 MSCE Neuglobsow RGM 0 10 20 30 40 50 60 11/1/1999 11/2/1999 11/3/1999 11/4/1999 11/5/1999 11/6/1999 11/7/1999 11/8/1999 11/9/1999 11/10/1999 11/11/1999 11/12/1999 11/13/1999 11/14/1999 Date pg/m 3 Obs Calc a CMAQ Neuglobsow RGM 0 10 20 30 40 50 60 70 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 pg/m 3 Obs Calc ADOM Neuglobsow RGM 0 10 20 30 40 50 60 70 11/1/99 11/2/99 11/3/99 11/4/99 11/5/99 11/6/99 11/7/99 11/8/99 11/9/99 11/10/99 11/11/99 11/12/99 11/13/99 11/14/99 Date pg/m 3 Obs Calc a EMAP Neuglobsow RGM 0 5 10 15 20 25 11/1/1999 11/2/1999 11/3/1999 11/4/1999 11/5/1999 11/6/1999 11/7/1999 11/8/1999 11/9/1999 11/10/1999 11/11/1999 11/12/1999 11/13/1999 11/14/1999 Date pg/m 3 Obs Calc a GRAHM Neuglobsow RGM 0 35 70 105 140 11/1/99 11/2/99 11/3/99 11/4/99 11/5/99 11/6/99 11/7/99 11/8/99 11/9/99 11/10/99 11/11/99 11/12/99 11/13/99 11/14/99 Date pg/m 3 Obs Calc a HYSPLIT Neuglobsow RGM 0 10 20 30 40 50 60 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 /99 pg/m 3 Obs Calc EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Budgets Dry Dep Wet Dep RGM Hg(p) Hg0 Chemistry Conclu- sions Stage III Stage II Stage I Intro- duction DEHM Neuglobsow RGM 0 6 12 18 24 30 11/1/1999 11/2/1999 11/3/1999 11/4/1999 11/5/1999 11/6/1999 11/7/1999 11/8/1999 11/9/1999 11/10/1999 11/11/1999 11/12/1999 11/13/1999 11/14/1999 Date pg/m 3 Obs Calc a Reactive Gaseous Mercury at Neuglobsow, Nov 1-14, 1999
  • 35. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 35 DE01 DE09 NL91 NO99 SE02 SE11 SE12 SE05 FI96 Monitoring Station 0.0 0.5 1.0 1.5 2.0 2.5 3.0 wet Hg deposition (g/km2-month) Obs MSCE-HM MSCE-HM-Hem HYSPLIT DEHM EMAP CMAQ August 1999 Mercury Wet Deposition
  • 36. 1. Atmospheric mercury modeling 3. What do atmospheric mercury models need? 2. Why do we need atmospheric mercury models? 4. Some preliminary results:  Model evaluation  Source Receptor Information 36
  • 37. Example of Detailed Results: 1999 Results for Chesapeake Bay 37
  • 38. Geographical Distribution of 1999 Direct Deposition Contributions to the Chesapeake Bay (entire domain) 38
  • 39. Geographical Distribution of 1999 Direct Deposition Contributions to the Chesapeake Bay (regional close-up) 39
  • 40. Geographical Distribution of 1999 Direct Deposition Contributions to the Chesapeake Bay (local close-up) 40
  • 41. Largest Regional Individual Sources Contributing to 1999 Mercury Deposition Directly to the Chesapeake Bay 41
  • 42. Largest Local Individual Sources Contributing to 1999 Mercury Deposition Directly to the Chesapeake Bay 42
  • 43. Emissions and Direct Deposition Contributions from Different Distance Ranges Away From the Chesapeake Bay 0 - 100 100 - 200 200 - 400 400 - 700 700 - 1000 1000 - 1500 1500 - 2000 2000 - 2500 > 2500 Distance Range from Chesapeake Bay (km) 0 20 40 60 80 Emissions (metric tons/year) 0 2 4 6 8 Deposition Flux (ug/m2-year) Emissions Deposition Flux 43
  • 44. Top 25 Contributors to 1999 Hg Deposition Directly to the Chesapeake Bay PhoenixServices BrandonShores StericycleInc. Morgantown ChalkPoint NASAIncinerator H.A.Wagner NorfolkNavyYard Hampton/NASAIncin. ChesapeakeEnergyCtr. Chesterfield Yorktown INDIAN RIVER Roxboro BALTIMORERESCO Mt. Storm Homer City Keystone BMWNC PossumPoint Montour PhoenixServices Belews Creek Harrisburg Incin. HarfordCo. Incin. MD MD MD MD MD VA MD VA VA VA VA VA DE NC MD WV PA PA NC VA PA MD NC PA MD 0% 20% 40% 60% 80% 100% Cumulative Fraction of Hg Deposition 0 5 10 15 20 25 Rank coal-fired elec gen other fuel combustion waste incineration metallurgical manufacturing/other 44
  • 45. Preliminary Results for other Maryland Receptors 45
  • 46. Maryland Receptors Included in Recent Preliminary HYSPLIT-Hg modeling (but modeling was not optimized for these receptors!) 46
  • 47. Largest Modeled Atmospheric Deposition Contributors Directly to Deep Creek Lake based on 1999 USEPA Emissions Inventory (national view) 47
  • 48. Largest Modeled Atmospheric Deposition Contributors Directly to Deep Creek Lake based on 1999 USEPA Emissions Inventory (regional view) 48
  • 49. Largest Modeled Atmospheric Deposition Contributors Directly to Deep Creek Lake based on 1999 USEPA Emissions Inventory (close-up view) 49
  • 50. Some Next Steps Expand model domain to include global sources Additional model evaluation exercises ... more sites, more time periods, more variables Sensitivity analyses and examination of atmospheric Hg chemistry (e.g. marine boundary layer, upper atmosphere) Simulate natural emissions and re-emissions of previously deposited Hg Use more highly resolved meteorological data grids Dynamic linkage with ecosystem cycling models 50
  • 51. Conclusions At present, many model uncertainties & data limitations Models needed for source-receptor and other info Monitoring data required to evaluate and improve models For this, simple may be better than complex measurements Some useful model results appear to be emerging Future is much brighter because of this coordination! 51
  • 54. • Hg is present at extremely trace levels in the atmosphere • Hg won’t affect meteorology (can simulate meteorology independently, and provide results to drive model) • Most species that complex or react with Hg are generally present at much higher concentrations than Hg • Other species (e.g. OH) generally react with many other compounds than Hg, so while present in trace quantities, their concentrations cannot be strongly influenced by Hg •The current “consensus” chemical mechanism (equilibrium + reactions) does not contain any equations that are not 1st order in Hg • Wet and dry deposition processes are generally 1st order with respect to Hg Why might the atmospheric fate of mercury emissions be essentially linearly independent? 54
  • 55. Spatial interpolation RECEPTOR Impacts from Sources 1-3 are Explicitly Modeled 2 1 3 Impact of source 4 estimated from weighted average of impacts of nearby explicitly modeled sources 4 55
  • 56. • Perform separate simulations at each location for emissions of pure Hg(0), Hg(II) and Hg(p) [after emission, simulate transformations between Hg forms] • Impact of emissions mixture taken as a linear combination of impacts of pure component runs on any given receptor 56
  • 57. “Chemical Interpolation” Source RECEPTOR Impact of Source Emitting 30% Hg(0) 50% Hg(II) 20% Hg(p) = Impact of Source Emitting Pure Hg(0) 0.3 x Impact of Source Emitting Pure Hg(II) 0.5 x Impact of Source Emitting Pure Hg(p) 0.2 x + + 57
  • 58. 58
  • 59. Standard Source Locations in Maryland region during recent simulation 59
  • 60. 0 50 100 150 200 250 300 350 day of year 0 10 20 30 40 50 60 70 80 90 100 ug/m2-year if daily dep continuted at same rate daily value weekly average Illustrative example of total deposition at a location ~40 km "downwind" of a 1 kg/day RGM source 60
  • 61. Eulerian grid models give grid-averaged estimates – …difficult to compare against measurement at a single location
  • 62. Geographic Distribution of Largest Anthropogenic Mercury Emissions Sources in the U.S. (1999) and Canada (2000) 62
  • 63. 63
  • 64. • In principle, we need do this for each source in the inventory • But, since there are more than 100,000 sources in the U.S. and Canadian inventory, we need shortcuts… • Shortcuts described in Cohen et al Environmental Research 95(3), 247-265, 2004 64
  • 65. Cohen, M., Artz, R., Draxler, R., Miller, P., Poissant, L., Niemi, D., Ratte, D., Deslauriers, M., Duval, R., Laurin, R., Slotnick, J., Nettesheim, T., McDonald, J. “Modeling the Atmospheric Transport and Deposition of Mercury to the Great Lakes.” Environmental Research 95(3), 247-265, 2004. Note: Volume 95(3) is a Special Issue: "An Ecosystem Approach to Health Effects of Mercury in the St. Lawrence Great Lakes", edited by David O. Carpenter. 65
  • 66. • For each run, simulate fate and transport everywhere, but only keep track of impacts on each selected receptor (e.g., Great Lakes, Chesapeake Bay, etc.) • Only run model for a limited number (~100) of hypothetical, individual unit-emissions sources throughout the domain • Use spatial interpolation to estimate impacts from sources at locations not explicitly modeled 66
  • 69. 69
  • 70. 70
  • 71. 71
  • 72. 72
  • 73. 0 - 15 15 - 30 30 - 60 60 - 120 120 - 250 distance range from source (km) 0.001 0.01 0.1 1 10 100 deposition flux (ug/m2-yr) Hg(II) emit, 50 m Hg(II) emit, 250 m Hg(II) emit, 500 m Hg(p) emit; 250 m Hg(0) emit, 250 m Source at Lat = 42.5, Long = -97.5; simulation for entire year 1996 using archived NGM meteorological data Deposition flux within different distance ranges from a hypothetical 1 kg/day source Hypothesized rapid reduction of Hg(II) in plumes? If true, then dramatic impact on modeling results…
  • 74. 0 - 15 15 - 30 30 - 60 60 - 120 120 - 250 distance range from source (km) 0 10 20 30 40 hypothetical 1 kg/day source deposition flux (ug/m2-yr) for Hg(II) emit Hg(p) emit Hg(0) emit Linear Why is emissions speciation information critical? 74
  • 75. Why is emissions speciation information critical? 0 - 15 15 - 30 30 - 60 60 - 120 120 - 250 distance range from source (km) 0 10 20 30 40 hypothetical 1 kg/day source deposition flux (ug/m2-yr) for Hg(II) emit Hg(p) emit Hg(0) emit Linear Logarithmic 0 - 15 15 - 30 30 - 60 60 - 120 120 - 250 distance range from source (km) 0.001 0.01 0.1 1 10 100 hypothetical 1 kg/day source deposition flux (ug/m2-yr) for Hg(II) emit Hg(p) emit Hg(0) emit 75
  • 76.  The form of mercury emissions (elemental, ionic, particulate) is often very poorly known, but is a dominant factor in estimating deposition (and associated source-receptor relationships)  Questions regarding atmospheric chemistry of mercury may also be very significant  The above may contribute more to the overall uncertainties in atmospheric mercury models than uncertainties in dry and wet deposition algorithms Emissions and Chemistry
  • 77. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 77 Neuglobsow Zingst Aspvreten Rorvik Mace Head
  • 78. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 78 Total Gaseous Mercury at Neuglobsow: June 26 – July 6, 1995 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 08-Jul 0.0 1.0 2.0 3.0 4.0 Total Gaseous Mercury (ng/m3) MEASURED NW NW NW N N S SE NW Neuglobsow
  • 79. EMEP Intercomparison Study of Numerical Models for Long-Range Atmospheric Transport of Mercury Intro- duction Stage I Stage II Stage III Conclu- sions Chemistry Hg0 Hg(p) RGM Wet Dep Dry Dep Budgets 79 Total Gaseous Mercury (ng/m3) at Neuglobsow: June 26 – July 6, 1995 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 MEASURED 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 MSCE Using default emissions inventory The emissions inventory is a critical input to the models… 26-Jun 28-Jun 30-Jun 02-Jul 04-Jul 06-Jul 0 1 2 3 4 MSCE - UBA Using alternative emissions inventory
  • 80. Some Additional Measurement Issues (from a modeler’s perspective) • Data availability • Simple vs. Complex Measurements • Process Information
  • 81. Process Information: 1. Dry Deposition - Resistance Formulation 1 Vd = --------------------------------- + Vg Ra + Rb + Rc + RaRbVg in which • Ra = aerodynamic resistance to mass transfer; • Rb = resistance of the quasi-laminar sublayer; • Rc = overall resistance of the canopy/surface (zero for particles) • Vg = the gravitational settling velocity (zero for gases).
  • 82. Dry Deposition  depends intimately on vapor/particle partitioning and particle size distribution information  resistance formulation [Ra, Rb, Rc...]  for gases, key uncertainty often Rc (e.g., “reactivity factor” f0)  for particles, key uncertainty often Rb  How to evaluate algorithms when phenomena hard to measure?
  • 83. Atmosphere above the quasi-laminar sublayer Quasi- laminar Sublayer (~ 1 mm thick) Surface Rb Rc Ra Very small particles can diffuse through the layer like a gas Very large particles can just fall through the layer In-between particles can’t diffuse or fall easily so they have a harder time getting across the layer Wind speed = 0 (?) Particle dry deposition phenomena
  • 84. 0.0001 0.001 0.01 0.1 1 10 100 particle diameter (microns) 1E-5 0.0001 0.001 0.01 0.1 1 Deposition Velocity (m/sec) Rb assumed small ( = 10 sec/m) Slinn and Slinn Typical Deposition Velocities Over Water with Different Rb Formulations Diffusion high; Vd governed by Ra Diffusion low; Settling velocity low; Vd governed by Rb Vd = settling velocity
  • 85. Process information needed: 1. For particle dry deposition, must have particle size distributions!
  • 86. LAKE ATMOSPHERE Pollutant on Suspended Sediment Pollutant Truly Dissolved in Water PROCESS INFORMATION: 2. The gas-exchange flux at a water surface depends on the concentration of pollutant in the gas- phase and the truly- dissolved phase (but these are rarely measured…) Gas-Phase Pollutant Particle-Phase Pollutant