Aerosol Properties over “Bright-Reflecting Source Regions ... · The aerosol characteristics used...
Transcript of Aerosol Properties over “Bright-Reflecting Source Regions ... · The aerosol characteristics used...
July 14, 2004UMBC/NASA GSFC 1N. Christina Hsu
Aerosol Properties over “Bright-Reflecting Source Regions”: The Deep Blue Algorithm and its
Applicability to MODIS
N. Christina Hsu andS.-C. Tsay, M. D. King, Y. J. Kaufman, J. R. Herman
University of Maryland, Baltimore County &NASA Goddard Space Flight Center
Greenbelt, Maryland USA
July 14, 2004UMBC/NASA GSFC 2N. Christina Hsu
TOMS Aerosol Index - time series
“2001 Perfect Dust Storm”
Asian Dust (+ microbes?): Long Range TransportSource Region
Dust Front
50 µm
Airborne Dusts
Sea of Japan4/9/2001
Dust layer NASA/GSFC4/14/2001
Dust layer
Dun-Huang, China4/6/2001
Dust layer
Lidar Profiling
July 14, 2004UMBC/NASA GSFC 3N. Christina Hsu
Rationale• Climate Forcing: requires aerosol properties near
source regions to achieve a complete picture of aerosol information from source to sink;
• Carbon Cycle: tracks iron sources from windblown dust for stimulating plankton growth in the open ocean;
• Aerosol Transport Modeling: needs accurate and realistic dust source locations; and
• Visibility and Adverse Health Effects: demands timely atmospheric turbidity information over affected regions.
July 14, 2004UMBC/NASA GSFC 4N. Christina Hsu
Percentage of Area Retrieved
by Current MODIS Aerosol
Algorithm[Chu et al., JGR, 2003]
(%)
Global Coverage forSurface Reflectance (2.1µm) >0.25
~15% � f(season) � ~25%
[Moody et al., 2004, in submission to IEEE TGRS]
Winter Spring
Summer Autumn
July 14, 2004UMBC/NASA GSFC 5N. Christina Hsu
•Simulated apparent 490 nm reflectance (atmosphere +ττττaerosol=1 + surface) at the top of the atmosph ere, as a function of surface reflectance.
•Non-absorbing aerosols make contrast apparent reflectancediminished faster for brighter surface.
•Absorbing aerosols make apparent reflectance brighter(or darker) for darker (or brighter) surface.
•The dash ed lines denote the critical values of surface reflectance where the presen ce of aerosol CANNOT be detected by that particular spectral wavelength.
Principle of Aerosol Retrievals*
Principle of Aerosol Retrievals*
*Hsu, Tsay, King, and Herman, 2004: Aerosol properties over bright-reflecting source regions, IEEE TGRS, 42, 557-569.
CSR
CSR = Critical surface reflectance
CSR
ττττ aerosol=1
ττττ aerosol=0
July 14, 2004UMBC/NASA GSFC 6N. Christina Hsu
MODIS Visible & NIR Bands:superimposed on the GOME spectral
reflectance taken over the Sahara
MODIS Visible & NIR Bands:superimposed on the GOME spectral
reflectance taken over the Sahara
412 nm
470nm
645 nm
July 14, 2004UMBC/NASA GSFC 7N. Christina Hsu
March 2001Gobi
Taklamaken
Inner Mongolia
African desert
July 14, 2004UMBC/NASA GSFC 8N. Christina Hsu
Inner Mongoliathen-farmland/grassland
(over-grazing and cultivation)
Gobi/Taklimakanaged deserts
Fine-grain sands
Coarse-size gravel
10 May 2001, 11:03 MTThe Great Gobi, Dunhuang, China
Nad
ir
July 14, 2004UMBC/NASA GSFC 9N. Christina Hsu
Maximum Likelihood Method
Dust Dominant
NO RETRIEVAL Yes
No
Surface ReflectanceDetermination
Smoke ModelSmoke ModelDust ModelDust Model
490, 670... nm SurfaceReflectivity (0.1ºx0.1º)
412 nm SurfaceReflectivity (0.1ºx0.1º)
412 nm SurfaceReflectivity (0.1ºx0.1º)
Flowchart for Deep Blue Algorithm
Radiances412, 490, 670 nm
Cloudy?
Cloud Screening or Cloud Mask Algorithm3x3 Pixels SpatialVariance at 412 nm
412/490 Absorbing Aerosol Index
Single-ScatteringAlbedo
Single-ScatteringAlbedo
Aerosol OpticalThickness
Aerosol OpticalThickness
+
AerosolType
ÅngströmExponent
ÅngströmExponent
+Aerosol OpticalThickness
Aerosol OpticalThickness
Mixed Aerosols
July 14, 2004UMBC/NASA GSFC 10N. Christina Hsu
Phase Function for Dust ModelPhase Function for Dust Model
July 14, 2004UMBC/NASA GSFC 11N. Christina Hsu
Deep Blue Algorithm for SeaWiFS/MODIS
Deep Blue Algorithm for SeaWiFS/MODIS
• Utilize solar reflectance at λ λ λ λ = 412, 490, and 670 nm to retrieve aerosol optical thickness (ττττa) and single scattering albedo (ωωωωo).• Less sensitive to aerosol height, compared to UV methods.• Works well on retrieving aerosol properties over various types of surfaces, including very bright desert.
ωωωω0(dust670nm)=1.0
ωωωωοοοο
ωωωωοοοο
ττττa
ττττa
July 14, 2004UMBC/NASA GSFC 12N. Christina Hsu
Asian Dust Outbreak6 April 2001
ê Deep Blue Algorithm:• Cloud mask works very well • Aerosol retrievals indicate dust
storms originated from Gobiand Inner Mongolia regions
• Single scattering albedos are quite different between thesetwo regions
SeaWiFS RGB - Rayleigh
0.0 1.0 2.0
SeaWiFS AOT
SSA (412nm)
0.85 1.00.90 0.95
July 14, 2004UMBC/NASA GSFC 13N. Christina Hsu
TOMS AI
1 Nov 2001
TOMS AI
8 May 2001 SeaWiFS RGB
AngstromExponentαααα
AngstromExponentαααα
τλ ∝ λ−α ,
α = lnτ1
τ 2
�
� � �
� � ln
λ2
λ1
�
� � �
� �
(Ångström 1961)
Kanpur
Kanpur
SeaWiFS αααα = -0.1AERONET αααα = 0.24
SeaWiFS αααα = 1.2AERONET αααα = 1.042
July 14, 2004UMBC/NASA GSFC 14N. Christina Hsu
Perfect Dust Storm7 April 2001
0.0 1.0 2.0
SeaWiFS AOT
ττττa
Angstrom exponent
0.0 1.0 2.0 αααα
July 14, 2004UMBC/NASA GSFC 15N. Christina Hsu
Comparisons with AOTfrom Sun Photometers
in China during ACE-Asia
Comparisons with AOTfrom Sun Photometers
in China during ACE-Asia
July 14, 2004UMBC/NASA GSFC 16N. Christina Hsu
Aerosol Optical Thickness Retrieved from Deep Blue Algorithm:Dust plumes in Africa
Aerosol Optical Thickness Retrieved from Deep Blue Algorithm:Dust plumes in Africa
ττττa
July 14, 2004UMBC/NASA GSFC 17N. Christina Hsu
Validation: Comparisons with AERONET Aerosol Optical Thickness
Validation: Comparisons with AERONET Aerosol Optical Thickness
North AfricaFebruary 2000
Arabian PeninsulaJune - July 2000
July 14, 2004UMBC/NASA GSFC 18N. Christina Hsu
0 0.5 1.0 1.5 2.0
Current MODISAerosol Optical Thickness
0.0 2.5 5.0 7.5 10
MODIS Deep BlueAerosol Index
1st Case: 6 April 2001MODIS Red-Green-Blue withRayleigh scattering removed
July 14, 2004UMBC/NASA GSFC 19N. Christina Hsu
SummarySummary
• It works!– Deep-Blue Algorithm well for SeaWiFS
measurements– Compared well with surface/aircraft products– Separate dust well from other anthropogenic
sources• We expect:
– Implement Deep-Blue Algorithm soon for MODIS– Produce new MODIS products over bright-
reflecting surfaces, and integrate into operational MODIS products
July 14, 2004UMBC/NASA GSFC 20N. Christina Hsu
Backup Slides
July 14, 2004UMBC/NASA GSFC 21N. Christina Hsu
Defined in a manner similar to the aerosol index for TOMS to distinguish between
absorbing and non-absorbing aerosols:
Imeas = Radiance measured by the satellite at 412 or 490 nm
Icalc = Radiance calculated using a radiative transfer model
Large AI’s are caused by high AOT or by highly absorbing aerosols.As with UV wavelengths, the visible AI is also a function of altitude.
Aerosol retrievals use an Aerosol Index:
Aerosol retrievals use an Aerosol Index:
AI = −100 ⋅ log10
I412
I490
� �
� �
meas
− log10
I412
I490
� �
� �
calc
�
� � �
� �
July 14, 2004UMBC/NASA GSFC 22N. Christina Hsu
The dependence of AI with both
AOT and absorption is confirmed by
simulations we performed using
aerosols of different types
*The properties of blue water were assumed in this simulation
Properties of Aerosol Index*
Properties of Aerosol Index*
July 14, 2004UMBC/NASA GSFC 23N. Christina Hsu
AerosolModel
ττττ412ττττ470
ττττ490ττττ470
Refractive Index412 nm
Refractive Index490 nm
ωωωω0412 nm
ωωωω0490 nm
DustSmoke
1.00 1.00 1.55 – 0.020i1.55 – 0.022i
1.55 – 0.008i1.55 – 0.026i
0.91 0.960.890.901.30 0.92
The aerosol characteristics used to generate the simulated radiances in these two figures are shown below
In areas of mixed aerosol types, we linearly mix radiances from the dust aerosol model, Rdust, with those from the smoke aerosol model,
Rsmoke = aRdust + (1-a)Rsmoke
Gaussian distribution with a peak at 3 km and a width of 1 km was assumed