THE OPTICAL PROPERTIES OF ATMOSPHERE DURING NATURAL FIRE EXPERIMENT IN CENTRAL RUSSIA AND THEIR IMPACT ON UV IRRADIANCE Nataly Ye. Chubarova Moscow State University, Geographical Department, Meteorological Observatory, email: [email protected]Alexei N. Rublev IMP, KURCHATOV Center, Moscow,Russia Allen R. Riebau USDA Forest Service Wildlife, Fisheries, Watershed and Air
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THE OPTICAL PROPERTIES OF ATMOSPHERE DURING NATURAL FIRE EXPERIMENT IN CENTRAL RUSSIA AND THEIR IMPACT ON UV IRRADIANCE Nataly Ye. Chubarova Moscow State.
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THE OPTICAL PROPERTIES OF ATMOSPHERE DURING NATURAL FIRE EXPERIMENT IN CENTRAL RUSSIA AND
THEIR IMPACT ON UV IRRADIANCE
Nataly Ye. ChubarovaMoscow State University, Geographical Department, Meteorological Observatory, email: [email protected]
Alexei N. RublevIMP, KURCHATOV Center, Moscow,Russia
Allen R. Riebau USDA Forest Service Wildlife, Fisheries, Watershed and Air Research Washington, DC
Meteorological parameters in summer-fall 2002 and climatic values (1960-1990):
june july august septembert_air,2002 17.8 23.4 17.9 12.5t_air_1960-1990 17 18.3 16.7 11.1precipitation,2002 50 16 51 72precipitation,1960-1990 78 91 79 63
30.07.02
Clear sky conditions
Average Aerosol Optical Thickness for 30.07.02: AOT_500=1.6
MOSCOWMoscow river
MO MSU
5.09.02
Average
AOT_500=1.72
CLEAR SKY FIRE SMOKE (1.08.02)
TAGANSKAYA SQUARE, MOSCOW
CLEAR SKY FIRE SMOKE, 4.09.02
(COURTESY OF ROBERT MUSSELMAN)
RED SQUARE, MOSCOW
AEROSOL OPTICAL THICKNESS IN MOSCOW AND MOSCOW SUBURBS (Zvenigorod) FROM CIMEL AND HAND
HELD HASEMETERS. MAY- SEPTEMBER 02.
00.20.40.60.8
11.21.41.61.8
22.22.42.62.8
33.23.43.6
24.0
4.02
27.0
4.02
30.0
4.02
03.0
5.02
06.0
5.02
09.0
5.02
12.0
5.02
15.0
5.02
18.0
5.02
21.0
5.02
24.0
5.02
27.0
5.02
30.0
5.02
02.0
6.02
05.0
6.02
08.0
6.02
11.0
6.02
14.0
6.02
17.0
6.02
20.0
6.02
23.0
6.02
26.0
6.02
29.0
6.02
02.0
7.02
05.0
7.02
08.0
7.02
11.0
7.02
14.0
7.02
17.0
7.02
20.0
7.02
23.0
7.02
26.0
7.02
29.0
7.02
01.0
8.02
04.0
8.02
07.0
8.02
10.0
8.02
13.0
8.02
16.0
8.02
19.0
8.02
22.0
8.02
25.0
8.02
28.0
8.02
31.0
8.02
03.0
9.02
06.0
9.02
09.0
9.02
12.0
9.02
15.0
9.02
18.0
9.02
21.0
9.02
24.0
9.02
27.0
9.02
30.0
9.02
AO
T 5
00
nm
AOT_500, MoscowAOT500, ZVEN HAZEAOT500, MOS HAZEmean AOT
Monthly mean aerosol optical thickness from Cimel in 2002 (in blue) and AOT retrieved from
actinometer following the method Yarkho& Tarasova [1991]
Effect of different gases on attenuation of Q erythema (dQe = Qe_gaz/ Qe_clear_from_all_gases,%)
observed in 2002 in clear sky conditions. Model simulations.
-45%
-40%
-35%
-30%
-25%
-20%
-15%
-10%
-5%
0%
0 0.5 1 1.5 2 2.5 3 3.5
AOT_380
dQe
due
to N
O2
-10%-9%-8%-7%-6%-5%-4%-3%-2%-1%0%
dQe
due
to H
CH
O,
O3,
S
O2
NO2 O3 HCHO SO2
Relative difference between Q erythema calculations with gaseous absorption (red
circles) and without it (black circles) and Qer measurements as a function of AOT. ho>25
degrees.The remaining dependence on AOT may be the indicator of
1. Less value of SSA?
2. Problems with non account of forward scattering at large AOT?
3. Larger gas concentration in upper troposphere or existence of other gas ?
-30%-20%-10%
0%10%20%30%40%50%60%70%80%
0 0.5 1 1.5 2 2.5 3 3.5
AOT380
Qer
_cal
c/Q
er_m
eas,
%
with SSA=0.9 o3no2 so2hcho out of gasincluding all gas
Relative difference between Q less 380nm calculations with gaseous absorption (red circles) and without it (black circles) and Q less 380nm measurements as a
function of AOT. ho>25 degrees.
10% of difference is in accordance with the difference in calibration factor CF utilized and CF obtained in Greece in 1999, which was not applied to these data.
NOTE THAT:NOTE THAT:
Brewer UV spectral measurements are lower than TOMS estimations [Fioletov et al., 2002]. Also there were different biases between TOMS and New Zealand (zero!) and European spectral measurements [MkKenzie et al., 2000]
-50%
-40%
-30%
-20%
-10%
0%
10%
20%
30%
40%
50%
0 0.5 1 1.5 2 2.5 3 3.5AOT_380
QU
V38
0_C
AL
C/Q
UV
380_
ME
AS Q UV less 380 with SSA=0.9
Q UV less 380 out of gasQ UV less 380 with NO2 account
Effect of diffuse irradiance to aerosol optical thickness underestimation
Close AOT values for NIP and A-50 and their difference from CIMEL sunphotometer MEAN the presence of coarse aerosol particles responsible for scattering in the instrument FOV.
00.20.40.60.8
11.21.41.61.8
22.22.4
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.6
АО
Т50
0
AOT_500нм,CIMEL
NIP 5.7 degrees
A-50 10 degrees
DIFFERENCE IN AOT = 0.2-0.7
Single scattering account in the instrument FOV:
w h e r e
b = 0 . 6 f o r C I M E L s u n p h o t o m e t e r b = 2 . 8 f o r E p p l e y p y r h e l i o m e t e r b = 5 f o r A - 8 0 ( R u s s i a n p y r h e l i o m e t e r )
)(
))(
(*expln'
_ Pm
DKKP
m
R
aaerRR
measaer
dxxPKb
RR 1
)cos(
)(2
dxxPKb
aa 1
)co s(
)(2
)exp(1 mD
Aerosol size distribution according to Dubovik&King retrieval method [2000] during clear
conditions (blue lines) and fires (red lines).
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.01 0.1 1 10 100RADII,MKM
dV
/dln
r
SMALL_FIRE_08.07.02 SMALL_FIRE_13.07.02
FIRE-30.07.02 FIRE_31.07.02
FIRE_1.08.02 FIRE_30.08
FIRE_02.09.02 FIRE_05.09.02
FIRE_07.09.02 CLEAR_02.07.02
CLEAR_21.08.02 CLEAR_12.09.02
The effect that may present due to forward scattering into the FOV.
-3 -2 -1 0 1 21E-9
1E-8
1E-7
1E-6
1E-5
1E-4
1E-3
0.01
0.1
1
dN(r
)/d
lg(r
), c
m-3
lg(r)-2 -1 0 1 2
1E-7
1E-6
1E-5
1E-4
1E-3
0.01
0.1
1
Rmax
= 15 m R
max=250 m
n(r)
lg(r)
Aerosol size distribution in Aerosol size distribution in aerosol continental model aerosol continental model ((WCP-112, 1986)WCP-112, 1986)::
Dust aerosol size distribution Dust aerosol size distribution model as a part of continental model as a part of continental model and when is cutted off at model and when is cutted off at 1515m:m:
This particle size, if exists in nature, may be responsible for large forward peak r 4.
Illustration:
The calculated difference between exact AOT and AOT’ measured in CIMEL FOV for continental type of aerosol at different airmass m.
1. The most severe natural fire event over Central Russia. AOT is more than 1.5-3 times larger than the monthly mean aerosol optical thickness in summer-fall 2002, reaching AOT_500>3.2. Flux validation approved that smoke aerosol has very slight absorption ( SSA0.95 from CIMEL retrievals). 3. In UV spectrum we should take into account the effects of gaseous absorption (mainly by NO2) both in clear sky and fire conditions. But sometimes other gases (O3, SO2) also play significant role. 4. NO2 may be responsible for the difference in comparisons of ground UV measurements with TOMS estimates especially in the polluted regions.5. It may be the effect of forward scattering into the CIMEL FOV due to the existence of large aerosol particles that is especially significant at high solar zenith angles. If they really present in nature? Need further studies..
Acknowledgements:We would like to thank:
1. AERONET team (Brent Holben, Alexander Smirnov, Oleg Dubovik, Ilya Slutsker, David Giles, etc.) for help in maintaining of measurements and providing a lot of consultations.
2. Moscow Ecological Monitoring Office for providing the data on concentration of some gas species and «PLANETA» Scientific Center for providing satellite images of fires around Moscow .
3. Dr. Wei Min Hao from USDA Forest Service for providing the Hasemeters for aerosol studies at Moscow suburbs.
4. NOAA for producing the backward trajectories over Moscow.
5. The staff of Meteorological observatory of MSU and, personally, V. Rozental’, N. Uliumdzhieva, A. Yurova, Ye. Stolyarova for technical help with instruments maintanence.
This work was done partially under the support of the USDA Forest Service in the frame of the project ‘‘Solar Radiation and Weather Variability Influences on Russian Sub-Boreal Forest Phenology.’’