1
Biomass burning plume impacts on photolysis frequencies and UV single scattering albedo during SEAC4RS 1. National Center for Atmospheric Research (NCAR), Boulder, CO 2. NASA Langley Research Center, Hampton, VA Abstract The 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 jO 1 D by as much as 95% and jNO 2 by 80%. Above the plume, jO 1 D was decreased while jNO 2 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. Hall 1 , K. Ullmann 1 , S. Madronich 1 , J.W. Hair 2 , M.A. Fenn 2 , C.F. Butler 2 , Bruce Anderson 2 , L. Ziemba 2 , A. Beyersdorf 2 CAFS Instrument Characterization 350 400 450 500 550 -0.4 -0.2 0 0.2 0.4 0.6 0.8 W avelength S hiftAnalysis W avelength (nm ) Offset(nm )and S pectra H ARP flux (scaled) ET flux(scaled) H A R P offset (nm ) 0 0.2 0.4 0.6 0.8 1 1.2 Angular R esponse for O ptic #21 R elative R esponse jO3 jNO2 jBr2 -100 -80 -60 -40 -20 0 20 40 60 80 100 0.9 0.95 1 1.05 1.1 R otation A ngle (deg) Relative R esponse jO3 jNO2 jBr2 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. jO 3 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 25.33 0 0.5 1 1.5 2 2.5 x 10 -6 20130826 N ASA D C -8 R F09 jO3 25.25 25.26 25.27 25.28 25.29 25.3 25.31 25.32 25.33 0 2 4 6 x 10 -3 jNO2 25.25 25.26 25.27 25.28 25.29 25.3 25.31 25.32 25.33 0 10 20 30 U TC hours Pitch/Roll (deg) cafs Ttl cafs dnw cafs upw cafs Ttl cafs dnw cafs upw Pitch Roll SZA ~ 78° 250 300 350 400 450 500 550 600 650 700 -1.5 -1 -0.5 0 0.5 1 1.5 N 02 field calibrations (Lam p G E07) W avelength (nm ) P ercentD ifference D O Y = 1 D O Y = 1 D O Y = 201 D O Y = 201 D O Y = 215 D O Y = 223 D O Y = 225 D O Y = 230 D O Y = 237 D O Y = 240 D O Y = 246 D O Y = 247 D O Y = 366 Discussion SEAC4RS 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 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 [O 3 O 2 +O( 1 D)] j [NO 2 NO+O( 3 P)] j [H 2 O 2 2OH] j [HNO 2 OH+NO] j [HNO 3 OH+NO 2 ] j [CH 2 O H+HCO] j [CH 2 O H 2 +CO] j [CH 3 CHO CH 3 +HCO] j [C 2 H 5 CHO C 2 H 5 +HCO] j [CHOCHO H 2 +2CO] j [CHOCHO CH 2 O+CO] j [CHOCHO HCO+HCO] j [CH3COCHO CH3CO+HCO] j [CH 3 COCH 3 CH 3 CO+CH 3 ] j [CH 3 OOH CH 3 O+OH] j [CH 3 ONO 2 CH 3 O+NO 2 ] j [CH 3 COCH 2 CH 3 CH 3 CO+CH2CH 3 ] j [CH 3 CH 2 CH 2 CHO C 3 H 7 +HCO] j [CH 3 CH 2 CH 2 CHO C 2 H 4 +CH 2 CHOH] j [HO 2 NO 2 HO 2 +NO 2 ] j [HO 2 NO 2 OH+NO 3 ] j [CH 3 CH 2 ONO 2 CH 3 CH 2 O+NO 2 ] j [Br 2 → Br+Br] j [BrO → Br+O] j [Br 2 O → products] j [BrCl → Br+Cl] j [HOBr → HO+Br] j [BrONO 2 → Br+NO 3 ] j [BrONO 2 → BrO+NO 2 ] j [Cl 2 → Cl+Cl] j [ClO → Cl+O( 3 P)] j [ClONO 2 → Cl+NO 3 ] j [ClONO 2 → ClO+NO 2 ] j [BrNO → Br+NO] j [BrONO → BrO+NO] j [BrONO → Br+NO 2 ] j [BrNO 2 → Br+NO 2 ] j [CHBr 3 → Products] j [ClNO 2 → Cl+NO 2 ] j [ClONO → Cl+NO 2 ] j [N 2 O 5 → NO 3 +NO 2 ] j [CH 3 CO(OONO 2 ) → CH 3 CO(OO) +NO 2 ] j [CH 3 CO(OONO 2 ) → CH 3 CO(O) +NO 3 ] j [CH 2 =C(CH 3 )CHO → Products] j [CH 3 COCH=CH 2 → Products] NEW REACTIONS Photolysis Frequencies 0 0.2 0.4 0.6 0.8 1 0 2000 4000 6000 8000 10000 12000 20130826 N ASA D C -8 R F09 C A FS /TU V A ltitude j(O 1 D) 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 jNO 2 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 14000 20130805 Longitude (deg) Altitude (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 M eas/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 21.8 3 3.5 4 4.5 x 10 -3 20130826 N ASA D C -8 R F09 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 1.7 x 10 -5 U TC hours jO3 cafs upw tuv upw Upwelling Upwelling impact +35% Total jNO2 impact +10% Upwelling impact -12% Total jO3 impact -5% Clea r Belo w 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 W avelength (nm ) C lear/(Sm oke orC loud)Ratio BB R im Fire (high above) BB R im Fire (in top) BB R im Fire (in deep) BB A ged (low /high A O D) BB A g1 (in) BB A g2 (in) C loud high alt(in) C loud high alt(above) C loud low alt(above) This study SEAC4RS CAFS 8/16/2013 Corr ARCTAS CAFS 4/17/2008 (selected points) Corr ARCTAS CAFS 6/29/2008 (selected points) Bais et al., 2014, doi:10.1039/c4pp90032d 300 350 400 450 500 0 0.5 1 1.5 2 2.5 3 x 10 14 W avelength (nm ) Flux (photons/nm /cm 2 /s) 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 Clear/Sm oke ratio ClearBelow Sm oke B elow Clear/Sm oke j(NO 2 ) j(O 1 D) Upwelling jNO 2 and jO 1 D 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

Biomass burning plume impacts on photolysis frequencies and UV single scattering albedo during SEAC4RS 1. National Center for Atmospheric Research (NCAR),

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Page 1: Biomass burning plume impacts on photolysis frequencies and UV single scattering albedo during SEAC4RS 1. National Center for Atmospheric Research (NCAR),

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