Climatology of Aerosol Optical Properties over the High Arctic ......Climatology of Aerosol Optical...
Transcript of Climatology of Aerosol Optical Properties over the High Arctic ......Climatology of Aerosol Optical...
Climatology of Aerosol Optical Properties over the High Arctic
Auromeet Saha1, N.T. O’Neill1, R.S. Stone2
K. Strong3, C. Viatte3, A. Herber4
1 CARTEL, Universite de Sherbrooke, Sherbrooke, Quebec, Canada2 CIRES/NOAA ESRL, Boulder, Colorado, USA
3 University of Toronto, Toronto, Ontario, Canada4 Alfred Wegener Institute for Polar & Marine Research, Germany
• Aerosols affect the Earth’s radiative balance through direct and indirect interactions with shortwave (SW) and longwave (LW) radiation at the top of the atmosphere, at the surface, as well as within the atmosphere by providing a radiative heating (or cooling) in the aerosol layers.
• Aerosols scatter (sulfates) and absorb (Soot/Black Carbon and Dust) the incoming solar radiation (Aerosol Direct Effect).
• Scattering aerosols reflect the incoming solar radiation resulting in atmospheric cooling. However, warming may result where the surface albedo is very high (Pueschel and Kinne, 1995) or if the sulfate is internally mixed with absorbing aerosols (Jacobson, 2001).
• Coarse mode aerosols such as mineral dust act like greenhouse gases by absorbing and emitting longwave (LW) radiation.
• Aerosols can influence the microphysical properties of clouds (Indirect aerosol effects) and thereby impacts the energy balance, precipitation, and the hydrological cycle. Depending on the composition and size, aerosols can serve as cloud condensation nuclei (CCN) or ice-forming nuclei (IN).
• Indirect effects of aerosols on cloud properties typically cause surface cooling (Quinn et al., 2008) but can also warm the surface through interactions with terrestrial (LW) radiation (Lubin and Vogelmann, 2006). The warming is expected to dominate during Arctic winter (Lubin and Vogelmann, 2007).
Introduction: Aerosols & Arctic Haze
• Long-range transport of pollution from mid-latitudes is a major source of aerosols to the Arctic, with a winter-spring maximum known as Arctic haze (Quinn et al., 2009). High aerosol concentrations in the Arctic during winter-spring can be due to efficient transport from mid-latitudes, reduced vertical mixing, and lack of precipitation (Shaw, 1995; Quinn et al., 2007; Garrett et al., 2010).
• Unlike long-lived CO2, aerosols have an average lifetime in the atmosphere from days to weeks, but exhibit a somewhat longer lifetime in the Arctic.
• Absorption of solar radiation by aerosols in the atmosphere is enhanced by highly reflective snow- and ice-covered surfaces in the Arctic. Deposition of light-absorbing aerosols (such as Soot) on snow or ice can decrease the surface albedo.
• The shortwave (SW) component of the energy balance can be affected by light absorbing aerosols through the atmosphere and in the ice/snow surface.
• With respect to the longwave (LW) component, the aerosol effect in the Arctic differs from other regions because of the cold atmospheric temperatures, frequent occurrences of temperature inversion, and low water vapor content.
• The longwave (LW) radiation plays a particularly important role in the energy balance in the Arctic because of prolonged polar nights with little or no sunlight.
• Hygroscopic growth of particles leads to absorption of terrestrial radiation, inducing a direct warming effect that can be particularly efficient during polar night (Ritter et al., 2005).
Introduction: Aerosols & Arctic Haze
High Arctic Sites
MODIS-Terra (250 m) July 8, 2004
OPAL
PEARL
Eureka
PEARL - Polar Environmental Atmospheric Research Lab. It is operated by the Canadian Network for the Detection of Atmospheric Change (CANDAC).
PEARL is located at Eureka, Nunavut (80N, 86W) on Ellesmere Island in Canada's high Arctic, 450 km north of Grise Fiord, the most northerly permanent settlement. PEARL is 1,100 km from the North Pole.
ØPAL - Zero altitude Polar Atmosphere Laboratory. It is located about 15 km southeast of the PEARL ridge lab which is at an elevation of 610 m.
PEARL
Instruments & Data used in this Study (Eureka)
Cimel Sun Photometer
Brewer SpectrometerBruker Fourier Transform Spectrometer
AHSRL
Cimel Sun Photometer (AEROCAN / AERONET)
Aerosol optical properties: Aerosol optical depth (AOD), and Effective radius of the fine & coarse mode.
The fine mode (f & reff,f) can typically be associated with forest or agriculture fire smoke, and pollution aerosols, while the coarse mode (c & reff,c) is an indicator of super-micron sized particulates such as dust, marine aerosols, and ice or water phase cloud particulates.
AEROCAN (Canadian Sunphotometer Network)
Resolute Bay
Saturna Island
Bratt’s Lake
Waskesiu
ChurchillKuujjuarapik
HalifaxSherbrookeEgbert
Pickle Lake
Fort McMurray
Kelowna
Chapais
Eureka (PEARL, OPAL)
Toronto
Yellowknife
Iqaluit
Sable Island
Lethbridge
AEROCAN is a full fledged sub-network of AERONET and benefits from all services that AERONET offers.
AEROCAN has a few unique features that go beyond AERONET protocols:
- All instruments use the high frequency, 3-minute mode (O’Neill mode).
- All data transmission is done using FTP.
- Complementary AOD processing chain in preparation for real timeingestion into an aerosol assimilation model (currently on hold).
- System wide display tools for real-time QA & troubleshooting.
- Separate prototype MySQL database for data QA (and science).
- Satellite calibration facility being developed (on hold with EC freezes).
AERONET vs AEROCAN
AEROCAN* (Canadian Starphotometer Sites)
Egbert
Eureka
Sherbrooke
Arctic High Spectral Resolution Lidar (AHSRL)
AHSRL measures the vertical profiles of backscatter coefficient () and depolarization ratio ()
The δ profiles permit one to distinguish between sub-micron smoke or pollution aerosols (low δ values) and irregularly shaped super-micron particles such as ice crystals and coarse mode aerosols such as dust (high δ values).
Bruker Fourier Transform Spectrometer(CO Column concentration)
Brewer Spectrometer (SO2)
Instruments & Data used in this Study (Barrow & Alert)
NOAA Sun Photometer SP02 used at Barrow & Alert (aerosol optical properties)
wavelength photometer deployedtraps heat and stabilizing temp
OPAL – CIMEL 327 PEARL – CIMEL 401
Sunphotometers installation in Eureka
runwayOPAL
PEARL Ridge Lab
This dual placement was designed to study the layer between the two sites as well as provide an element of redundancy for the AOD measurements.
OPAL
PEARL
~12 km~0.61 km
SAFFIRE
OPALPEARL
0.00
0.04
0.08
0.12
0.16
AO
D (5
00 n
m)
OPALPEARL
Eureka Aerosol Optical Depth Climatology
2007-2011
0
50
100
150
MAR APR MAY JUN JUL AUG SEP
Nob
s (D
ays)
OPALPEARL
0.00
0.05
0.10
0.15
0.20
0.25
AO
D (5
00 n
m)
Egbert (1998-2011)
CARTEL(1995-2010)
0
100
200
300
JAN
FEB
MAR AP
R
MAY JU
N
JUL
AUG
SEP
OC
T
NO
V
DEC
N obs
(Day
s) EgbertCARTEL
Mid-Latitude AOD Climatology
0.00
0.50
1.00
1.50
2.00
Prec
ipita
ble
Wat
er (c
m)
OPALPEARL
0
50
100
150
MAR APR MAY JUN JUL AUG SEP
Nob
s (D
ays)
OPALPEARL
Eureka Precipitable Water Climatology
0
1
2
3
Prec
ipita
ble
Wat
er (c
m)
Egbert (1998-2011)
CARTEL (1995-2010)
0
100
200
300
JAN MAR MAY JUL SEP NOV
Nob
s (D
ays)
EgbertCARTEL
Mid-latitude Precipitable Water Climatology
0.00
0.05
0.10
0.15
0.20
N L N L N L N L N L
AO
D (5
00 n
m)
OPAL
PEARL
0
10
20
30
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
Nob
s (D
ays) OPAL
PEARL
2007 2008 2009 2010 2011
Seasonal and inter-annual variation of AOD over EurekaBiomass burning from Forest & Agricultural Fires in Russia & Kazakstan
Kasatochi volcanic aerosols
Sarychev volcanic aerosols
Biomass burning aerosols during Spring 2008 (ARCTAS)*
*Saha et al., GRL, 2010
0.0
0.1
0.2
0.3
0.4
9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25
PEARL (Level 1.0), poly. order = 2, = 0.5 m
Total Fine Coarse
m-1 str-1)
Day of Month (April 2008)
Alti
tude
(km
)A
ltitu
de (k
m)
AHSRL aerosol backscatter cross section ()
AHSRL particulate circular depolarization ratio ()
Fine mode aerosols were associated with biomass burning (agricultural and forest fires) from E/SW Russia & northenKazakhstan.
Coarse‐mode events were likely due to ice particles whose nucleation may have been associated with the presence of smoke, or possibly dust.
f correlates well with variations in the presence of small , while cvalues correlate with in the presence of large .
Barrow
T hule
PEA RL
Yellowknife
Ny-A lesund
Hornsund
SERb
(c)
Ka(e)
(b)(a)
(e)2008 04 12 1500 UTC 2008 04 28 1800 UTC
SERaKb
SER2
2008 04 24 0900 UTC
SER2
*Saha et al., GRL, 2010
AOD
GEM-AQ AOD simulation for April 2008
*Saha et al., GRL, 2010
0
0.1
0.2
0.3
103.4 103.5 103.6 103.7 103.8 103.9 104 104.1
f ine mode OD
coarse mode OD
total OD
0
0.1
0.2
0.3
104.4 104.5 104.6 104.7 104.8 104.9 105 105.1
f ine mode OD
coarse mode OD
total OD
April 12 April 13
Fine Mode (smoke) event of April 12-13 observed at Eureka
fine modeSmoke layers
*Saha et al., GRL, 2010
Aqua, April 12, 1405 UT ThuleEureka
Terra - fusion of April 12, 1155 and 1200 UT images.
MODIS true color images (fusion of Terra and Aqua) showing the Pan-Arctic view of the April 12 plume crossing Eureka (part of the SERa plume movement).
MODIS Imagery for April 12 Smoke Plume crossing Eureka
*Saha et al., GRL, 2010
Ny-Alesund
MODIS Aqua Visible, 0930, April 24, 2008, 500 m. resolution
Smoke surrounding Ny-Alesund (Kb event of April 24). While blinking between the Aqua visible image (R,G, B = bands 1, 4, 3) and the Aqua SWIR image (R,G, B = bands 7, 2, 1), the fine-mode smoke largely disappears in the SWIR image over water.
Ny-Alesund
MODIS Imagery for April 24 Fine Mode Event at Ny-Alesund
*Saha et al., GRL, 2010
Smoke plume event at Barrow. The Aqua true-color image has been CMYK enhanced (linear stretch applied to the C, M, Y channels). The higher reflectivity of clouds versus snow indicates that the plume lies above a low-lying cloud. This was confirmed in comparisonswith the HSRL data of Ferrare et al. (2009). The red circle indicates the position of Barrow.
MODIS Aqua Visible, 2220, April 19, 2008, 250 m. resolution
MODIS Imagery for April 19 Fine Mode Event at Barrow (Alaska)
*Saha et al., GRL, 2010
108 109 110 111
0.0
0.1
0.2
0.3
0.4
0.5
0.6
Aeronet Level 1.0
D f Y (2008)
17-19 Apr-2008PEARL
AOT
()
Total Fine Coarse
HYSPLIT Back Trajectories
OMI Aerosol Index Gobi Desert
CALIOP profiles of Total Attenuated Backscatterand depolarization ratio
Coarse Mode Event observed at Eureka during April 17-19
For this high event, c varies in a low frequency (diurnal) fashion, unlike typical cloud effects whose high frequency cexcursions form the basis of most cloud screening algorithms. The smoke plume positions inferred from MODIS imagery and synoptic- dynamics combined with an analysis of the lidar / sunphotometry data and AOD simulations by Pierce et al. (2009) suggest that these features were a complex mixture of smoke and ice crystals and that the smoke particles (or possibly dust) might have acted as Ice Nuclei.
Eureka
Precipitating Ice Crystals
100.5 100.6 100.7 100.8 100.9 101.0 101.1 101.2 101.3
0.0
0.1
0.2
0.3
0.4
0.5
Barrow (Screened), poly. order = 2, = 0.5 m
Total Fine Coarse
The AOD time series plot over Barrow on April 9 shows significant low-frequency c variation with enhanced backscatter and high cross-polarization profiles. Using airborne lidar measurements acquired near Barrow on April 9, Ferrare et al. (2009) concluded that ice particles were making a significant contribution to the AOD.
Coarse Mode Event observed at Barrow on April 9
*Saha et al., GRL, 2010
0
0.2
0.4
182.0 182.5 183.0 183.5 184.0
Opt
ical
Dep
th
fine mode ODcoarse mode OD
total ODAHSRL SOD
0.0
0.2
0.4
182.0 182.5 183.0 183.5 184.0Doy.UT/24
Opt
ical
Dep
th
0
5
10
SO2 [
DU
]fine mode ODBrewer #007Brewer #021Brewer #069
m-1 str-1)
July 1 July 2
(d)
(a)
(b)
(c)
Sarychev volcanic aerosols over the Arctic during Summer 2009*
0.00
0.05
0.10
0.15
f (5
00 n
m)
Pre-eruption Post-eruption
0.0
0.1
0.2
0.3
0.4
r eff
,f [
m]
*O’Neill et al., JGR 2012
Pre- and post- SAT f, and reff,f for four AEROCAN / AERONET high-Arctic stations
0PAL PEARL Thule Hornsund
Eureka
July 01, 2009 OMI: July 02, 2009
CA
LIO
P –
stra
tosp
heric
O
DO
MI –
colu
mn
conc
entra
tion
Envelope of CALIOP orbit lines
0.0
0.5
1.0
1.5
2.0SO2 [DU]
Illustration of Sarychev Plume (OMI SO2 vs CALIOP SOD)
*O’Neill et al., JGR 2012
1000
1500
2000
2500
CO
[mol
. cm
-2] x
1015
0
10
20
30
Nob
s (D
ays)
Variations of CO Total Column over Eureka
0
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
MA
R
AP
R
MA
Y
JUN
JUL
AU
G
SE
P
2007 2008 2009 2010 2011
CO being a tracer of biomass, one would expect a degree of correlation with the fine mode aerosols that are also a primary product of biomass burning.
y = 0.0027e0.0014x
R2 = 0.5781
0
0.1
0.2
0.3
1000 1500 2000 2500 3000
CO Column [mol. cm-2] x 1015
f (5
00 n
m)
2007
y = 0.0003e0.0026x
R2 = 0.7209
0
0.1
0.2
0.3
1000 1500 2000 2500 3000
CO Column [mol. cm-2] x 1015
f (5
00 n
m)
2008
y = 0.0099e0.001x
R2 = 0.5884
0
0.1
0.2
0.3
1000 1500 2000 2500 3000CO Column [mol. cm-2] x 1015
f (5
00 n
m)
2009
Sarychev
Fine Mode AOD vs CO
Shown in the figures are the variation of fine-mode AOD as a function of CO concentration for the three years of 2007, 2008 and 2009.
One can observe a moderate (2007), strong (2008) and insignificant (2009) correlation respectively for these three years. However if we separate out the Sarychev fine-mode AODs from the 2009 regression, we find a R2 value that is comparable to the other two years.
0.00
0.05
0.10
0.15
AOD
(500
nm
)
totalfine modecoarse mode
0.0
0.1
0.2
0.3
r eff,
f (m
)
PEARL
0
1
2
3
MAR MAY JUL SEP MAR MAY JUL SEP MAR MAY JUL SEP MAR MAY JUL SEP MAR MAY JUL SEP
r eff,
c (
m)
PEARL
Retrievals of fine & coarse mode AOD and Effective radius
2007 2008 2009 2010 2011
The fine-mode AOD shows the spring to summer decrease (confirms that the total AOD is fine-mode dominated).
The coarse mode AOD shows apparent springtime activity that could possibly be Asian Dust.
The fine-mode effective radius shows a relatively consistent variation except in 2009 where we know there was a strong Sarychev influence (O’Neill et al., 2012).
The coarse mode effective radius shows significant variations that could be real (possibly associated with marine aerosols) but which might, just as well, be associated with low-AOD retrieval artifacts.
reff,f ~ 0.2 m
00 04 08 12 16 20 24
0.00
0.05
0.10
0.15
0.20
0.25
Time (GMT)
AOT
()
Total Fine Coarse
Taklimakan Desert April 19, 2009
Illustration of Coarse Mode Event (Asian Dust)
Precipitating Ice crystals
Dust
April 27, 2009
0.0
0.2
0.4
0.6
0.8
18 19 20
AHSRL, = 532 nm, Fine: 0.05 < < 0.4, Coarse: > 0.4
Fine Coarse
Fine Coarse
PEARL (Level 1.0), poly. order = 2, = 0.5 m
April 2008
Coarse Mode Event (Nucleation of Smoke & Dust) during ARCTAS*
*Saha et al., GRL, 2010
0.0
0.1
0.2
0.3
0.4
16 17 18 19 20 21 22 23 24 25 26 27 28 29 30
PEARL (Level 1.0), poly. order = 2, = 0.5 m
April 2009
Total Fine Coarse
Suspicious coarse mode peaks possibly due to frost in the Cimeloptics.
Coarse mode event at PEARL (Artifacts)
AHSRL does not show any coarse mode event
Frost Issues
Cimel SunphotometerSept. 9, 2011
Cimel SunphotometerSept. 22, 2009
Star PhotometerWinter 2012
0
0.2
0.4
0.6
0.8
1
14 15 16 17 18 19
fine mode OD coarse mode OD total OD
-10
10
30
50
14 15 16 17 18 19
day in April, 2008
100*[L(sky)-L(ext.)]/L(ext) at 1020, 870, 675 and 440 nm
Almucantar % differences,
Almucantar radiance differences at 6° azimuth shouldagree within 5%.
y = 0.9659x + 0.1163R2 = 0.8315
y = 1.7528x + 0.0893R2 = 0.7687
y = 1.8462x + 0.348R2 = 0.2402
0
0.5
1
1.5
2
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 11 / m
AO
T(50
0 nm
)
April 15April 16April 14Linear (April 16)Linear (April 15)Linear (April 14)
Computed AOT varies suspiciously as 1 / m(m – airmass)
April 2008
Coarse mode event at Thule (Artifacts)
0
10
20
Jan Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec
Win
d Sp
eed
(km
hr-1
)
Climate Normals (1971-2000)
Coarse Mode Retrievals vs Wind speed (Eureka)
0
1
2
3
MAR MAY JUL SEP MAR MAY JUL SEP MAR MAY JUL SEP MAR MAY JUL SEP MAR MAY JUL SEP
r eff,
c (
m)
PEARL
Eureka (OPAL) Wind Speed Climatology2007 2008 2009 2010 2011
Sunphotometry at High Arctic Sites
Barrow-NOAA
Barrow-AERONET PEARL
OPALThule
Resolute Bay
Alert
HornsundNy-Alesund
Kangerlussuaq
Pan-Arctic sites for the AOD Climatology
0.00
0.05
0.10
0.15
0.20
AO
D (5
00 n
m)
Barrow NOAA (2001-2011)Barrow AERONET (1999-2011)Resolute Bay (2004-2011)OPAL (2007-2011)PEARL (2007-2011)Alert (2004-2011)Thule (2007-2011)Kangerlussuaq (2008-2011)Hornsund (2006-2011)Ny-Alesund (1991-2011)
gy
0
100
200
300
MAR APR MAY JUN JUL AUG SEP OCT
Nob
s (D
ays)
Barrow NOAABarrow AERONETResolute BayOPALPEARLAlertThuleKangerlussuaqHornsundNy-Alesund
Pan-Arctic AOD Climatology
AOD monthly climatology for an enhanced number of high Arctic stations on a pan-Arctic scale. It simultaneously shows the spring to summer decrease noted for Eureka as well as a west to east AOD decrease.
Summary & Conclusions
A multi-year AOD and effective radius climatology for the high Arctic showed a number of consistent features:
Spring to summer decrease of fine-mode AOD (probably attributable to biomass burning and/or anthropogenic pollution).
Significant correlation of fine mode AOD with CO concentration (which indicates a predominance of biomass burning aerosols throughout the entire year).
West to east decrease in AOD on a pan-Arctic scale.
Acknowledgements
0.00
0.05
0.10
0.15
0.20
07-May 21-May 04-Jun 18-Jun 02-Jul 16-Jul 30-Jul 13-Aug 27-Aug
AO
D (5
00 n
m)
OPAL
PEARL
2011
Differential Sunphotometry at Eureka