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Biomass burning plume impacts on photolysis frequenciesand UV single scattering albedo during SEAC4RS
1. National Center for Atmospheric Research (NCAR), Boulder, CO 2. NASA Langley Research Center, Hampton, VA
AbstractThe Studies of Emissions and Atmospheric Composition, Clouds and
Climate Coupling by Regional Surveys (SEAC4RS) campaign during the summer of 2013 was strongly impacted by biomass burning (BB) from western U.S. fires. Scattering and absorption by particles in the plume directly impact spectral actinic flux which drives the photochemistry. Near the fire, high absorption results in reduced UV-B flux. In combination with strong plume convection (including pyro-convection), this permits injection of volatile, normally short-lived species to the free troposphere and beyond. Measurements from the Charged-coupled device Actinic Flux Spectroradiometers (CAFS) onboard the NASA DC-8 aircraft show penetration of the California Rim fire reduced in situ jO1D by as much as 95% and jNO2 by 80%. Above the plume, jO1D was decreased while jNO2 increased. Calculation of UV single scattering albedo (SSA) suggests organic carbon aerosols increase absorption in the UV-B in a wide variety of BB plumes. Downstream, the aged plume may contain more strongly scattering particles due to hygroscopic growth. Enhanced photolysis has been theorized, but conclusive evidence is elusive.
Optical Collector
Detector and Electronics
S. R. Hall1, K. Ullmann1, S. Madronich1, J.W. Hair2, M.A. Fenn2, C.F. Butler2 , Bruce Anderson2, L. Ziemba2, A. Beyersdorf2
CAFS Instrument Characterization
350 400 450 500 550
-0.4
-0.2
0
0.2
0.4
0.6
0.8Wavelength Shift Analysis
Wavelength (nm)
Offs
et (
nm
) a
nd
Sp
ect
ra
HARP flux (scaled)ET flux (scaled)HARP offset (nm)
-100 -80 -60 -40 -20 0 20 40 60 80 1000
0.2
0.4
0.6
0.8
1
1.2Angular Response for Optic #21
Re
lativ
e R
esp
on
se
jO3jNO2jBr2
-100 -80 -60 -40 -20 0 20 40 60 80 1000.9
0.95
1
1.05
1.1
Rotation Angle (deg)
Re
lativ
e R
esp
on
se
jO3jNO2jBr2
Determination of instrument wavelength offsets by comparison to features in the extraterrestrial solar flux spectrum (Slaper et al., GRL 22, 1995).
Angular response of the zenith optic optimized for a hemispherical response. Azimuthal response not shown.
Demonstration of combined nadir and zenith angular response quality of the optics at high solar zenith angle (low sun). Roll maneuvers have minimal effect on the total actinic flux, except when the sun approaches 90° relative to the optics. jO3 is less directionally impacted due to a higher sensitivity to diffuse, scattered light.
CAFS field spectral response calibration history demonstrating instrument stability throughout the campaign.
Laboratory stray light characterization by long pass filter analysis to assign spectral corrections. Note the structure in HARP is not evident in the CAFS system.
25.25 25.26 25.27 25.28 25.29 25.3 25.31 25.32 25.330
0.5
1
1.5
2
2.5x 10
-6 20130826 NASA DC-8 RF09
jO3
25.25 25.26 25.27 25.28 25.29 25.3 25.31 25.32 25.330
2
4
6
x 10-3
jNO
2
25.25 25.26 25.27 25.28 25.29 25.3 25.31 25.32 25.33
0
10
20
30
UTC hours
Pitc
h/R
oll (
deg)
cafs Ttlcafs dnwcafs upw
cafs Ttlcafs dnwcafs upw
PitchRoll
SZA ~ 78°
250 300 350 400 450 500 550 600 650 700-1.5
-1
-0.5
0
0.5
1
1.5N02 field calibrations (Lamp GE07)
Wavelength (nm)
Pe
rce
nt D
iffe
ren
ce
DOY = 1DOY = 1DOY = 201DOY = 201DOY = 215DOY = 223DOY = 225DOY = 230DOY = 237DOY = 240DOY = 246DOY = 247DOY = 366
DiscussionSEAC4RS provided a rich database for study of photolysis
frequencies in the presence of BB aerosols. While actinic flux measurements are not ideal for aerosol characterization, CAFS provided the opportunity to determine extinction trends in the UV-B where few other measurements exist. UV-B deviations have strong implications for photochemistry, aerosol lifetimes (photofragmentation) and human health and agriculture.
The TUV—CAFS determined SSA trend provides strong evidence for higher absorption in the UV-B. Black carbon is expected to have relatively flat or decreasing absorption in the UV. Thus the decreasing SSA is most likely due to absorption by plentiful organic carbon in the plumes.
Evidence of enhanced photolysis above aged BB plumes due to hygroscopic growth was not clearly established. However, small enhancement is difficult to detect due to variability in SSA, AOD, albedo, humidity, ozone columns and, most significantly, clouds.
Further study:• Additional case studies to determine aerosol optical
properties above, within and below aerosol layers.• Apply the determined UV-B SSA dependence to the TUV model
to assess flux and photolysis profiles.• Apply results in regional chemistry models to assess the
regional photochemical impact.
Acknowledgements: NCAR is operated by the University Corporation for Atmospheric Research under the sponsorship of the National Science Foundation (NSF). The SEAC4RS research was funded by NASA under award No. NNX12AB82G S01 and NSF. Special thanks to all SEAC4RS collaborators and logistic team members.
j [O3 → O2+O(1D)]
j [NO2 → NO+O(3P)]
j [H2O2 → 2OH]
j [HNO2 → OH+NO]
j [HNO3 → OH+NO2]
j [CH2O → H+HCO]
j [CH2O → H2+CO]
j [CH3CHO → CH3+HCO]
j [C2H5CHO → C2H5+HCO]
j [CHOCHO → H2+2CO]
j [CHOCHO → CH2O+CO]
j [CHOCHO → HCO+HCO]
j [CH3COCHO → CH3CO+HCO]j [CH3COCH3 → CH3CO+CH3]
j [CH3OOH → CH3O+OH]
j [CH3ONO2 → CH3O+NO2]
j [CH3COCH2CH3 → CH3CO+CH2CH3]
j [CH3CH2CH2CHO → C3H7+HCO]
j [CH3CH2CH2CHO → C2H4+CH2CHOH]
j [HO2NO2 → HO2+NO2]
j [HO2NO2 → OH+NO3]
j [CH3CH2ONO2 → CH3CH2O+NO2]
j [Br2 → Br+Br]
j [BrO → Br+O]j [Br2O → products]
j [BrCl → Br+Cl]
j [HOBr → HO+Br] j [BrONO2 → Br+NO3]
j [BrONO2 → BrO+NO2]
j [Cl2 → Cl+Cl]
j [ClO → Cl+O(3P)]j [ClONO2 → Cl+NO3]
j [ClONO2 → ClO+NO2]
j [BrNO → Br+NO]
j [BrONO → BrO+NO]
j [BrONO → Br+NO2]
j [BrNO2 → Br+NO2]
j [CHBr3 → Products]
j [ClNO2 → Cl+NO2]
j [ClONO → Cl+NO2]
j [N2O5 → NO3+NO2]
j [CH3CO(OONO2) → CH3CO(OO)+NO2]
j [CH3CO(OONO2) → CH3CO(O)+NO3]
j [CH2=C(CH3)CHO → Products]
j [CH3COCH=CH2 → Products]
NEW REACTIONS
Photolysis Frequencies
0 0.2 0.4 0.6 0.8 10
2000
4000
6000
8000
10000
1200020130826 NASA DC-8 RF09
CAFS/TUV
Alti
tud
e
j(O1D)j(NO
2)
Fresh Rim fire aerosol loading
Biomass burning absorption
Actinic flux was modeled using a modified NCAR Tropospheric Ultraviolet and Visible (TUV) radiative transfer model version 5.1. CAFS and TUV were processed for photolysis frequencies using identical calculations to ensure the same geographic, thermal and molecular parameters were applied to the measured and modeled spectra. BB plume from NASA DIAL (above) indicating high aerosol below 6 km and (right) comparison with a clean air profile shaded with the CAFS/TUV jNO2 ratio. Hygroscopic scattering enhancement above the aged plume is not evident in the dry, clear conditions
-118.2 -118 -117.8 -117.6 0
2000
4000
6000
8000
10000
12000
1400020130805
Longitude (deg)
Alti
tude
(m)
0.75
0.8
0.85
0.9
0.95
1
-104.4 -104.2 -104 -103.8 -103.6 -103.4
20130816
Longitude (deg)
jNO
2 Mea
s/M
odel
0.75
0.8
0.85
0.9
0.95
1
Aged BB plume
Low Aerosol
Search for aerosol enhanced scattering
Three BB plume flights with SSA determined by NASA LARGE and spectrally with TUV regression to match the CAFS actinic flux
UV-SSA determined from actinic flux
21.3 21.35 21.4 21.45 21.5 21.55 21.6 21.65 21.7 21.75 21.83
3.5
4
4.5
x 10-3 20130826 NASA DC-8 RF09
jNO
2
21.3 21.35 21.4 21.45 21.5 21.55 21.6 21.65 21.7 21.75 21.8
1.1
1.2
1.3
1.4
1.5
1.6
1.7x 10
-5
UTC hours
jO3
cafs upwtuv upw
Upwelling
Upwelling impact +35%Total jNO2 impact +10%
Upwelling impact -12%Total jO3 impact -5%
Clear Below
Rim Fire Below
Aged biomass burning SSA in comparison with UV ground station and ARCTAS/CAFS determinations
300 320 340 360 380 400 420 440 460 480 500
0.5
1
1.5
2
2.5
3
Wavelength (nm)
Cle
ar
/ (S
mo
ke o
r C
lou
d)
Ra
tio
BB Rim Fire (high above)BB Rim Fire (in top)BB Rim Fire (in deep)BB Aged (low/high AOD)BB Ag1 (in)BB Ag2 (in)Cloud high alt (in)Cloud high alt (above)Cloud low alt (above)
This study SEAC4RS CAFS 8/16/2013Corr ARCTAS CAFS 4/17/2008 (selected points)Corr ARCTAS CAFS 6/29/2008 (selected points)
Bais et al., 2014, doi:10.1039/c4pp90032d
300 350 400 450 5000
0.5
1
1.5
2
2.5
3
x 1014
Wavelength (nm)
Flu
x (p
hoto
ns/n
m/c
m2 /s
)
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
Cle
ar/S
mok
e ra
tio
Clear BelowSmoke BelowClear/Smoke
j(NO2)j(NO2)
j(O1D)j(O1D)
Upwelling jNO2 and jO1D as the DC-8 aircraft transitions from clear skies below to Rim Fire BB plume overflight. Note the opposing trend of the photolysis frequencies.
Spectral upwelling actinic flux over clear and smoke regions of the Rim Fire. The flux ratio indicates enhanced UV absorption by brown carbon aerosols in the biomass burning plume.
Ratio of clear/smoke or clear/cloud under varying conditions indicating consistency in the brown carbon enhanced UV absorption in BB and clouds dominated by scattering.
Corr et al., doi:10.5194/acp-12-10505-2012