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The effect of Brown Carbon on thermal-optical analysis: a correction based on optical multi-wavelength analysis

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Sunset EC/OC analyzer  Elemental, Organic and Total Carbon.

HPLC – PAD  Levoglucosan.

AMS 

14

C for quantification of Modern and Fossil Carbon.

MWAA

 Aerosol Absorption coefficient @ 5l: 375, 407, 532, 635 and 850nm.

Bibliography

Massabò D, Bernardoni V, Bove MC, Brunengo A, Cuccia E, Piazzalunga A, Prati P, Valli G, Vecchi R. (2013). A Multi-wavelength optical set-up for the characterization of carbonaceous particulate matter, Journal of Aerosol Science, 60, 34-46.

Massabò, D, Caponi, L, Bernardoni, V, Bove, MC, Brotto, P, Calzolai, G, Cassola, F, Chiari, M, Fedi, ME, Fermo, P, Giannoni, M, Lucarelli, F, Nava, S, Piazzalunga, A, Valli, G, Vecchi, R, Prati, P, (2015). Multi-wavelength optical determination of black and brown carbon in

atmospheric aerosols, Atmospheric Environment, 108, 1-12.

Massabò D, Caponi L, Bove, MC, Prati P, (2016). Brown Carbon and thermal-optical analysis: A correction based on optical multi-wavelength apportionment of atmospheric aerosols, Atmospheric Environment, 125, 119-125.

The effect of Brown Carbon on thermal-optical analysis: a correction based on

optical multi-wavelength analysis

D. Massabò

1

, V. Bernardoni

2

, M. C. Bove

1

, L. Caponi

1

, G. Valli

2

, R. Vecchi

2

, P. Prati

1

1: Dept. of Physics, University of Genoa & INFN Via Dodecaneso 33, 16146, Genova, Italy 2: Dept. of Physics, Università degli Studi di Milano & INFN Via Celoria 16, 20133, Milano, Italy

Motorized stage: l selection 16 positions filter wheel Photodiodes Stepper motors: filter selection and scanning 5 LASER diodes: 375nm 407nm 532 nm 635nm 850 nm

D. Massabò et al., JAS:60:34-46, 2013

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 07/11/2014 16/11/2014 25/11/2014 04/12/2014 13/12/2014 22/12/2014 31/12/2014 A A E babs [ Mm -1 ] @6 35 nm Date

b_abs BCff b_abs BCwb b_absBrC AAE

y = 2.39x + 0.05 R² = 0.96 0.0 0.2 0.4 0.6 0.8 1.0 0.00 0.10 0.20 0.30 0.40 B a bs BrC (Mm -1 ) @63 5n m Levoglucosan (mg m-3)

Absorption coefficient apportioned to BrC vs. Levoglucosan concentration BrC BC

b

a

b

b

b

b

abs

BrC

abs

BC

abs

abs

l

l

l

l

l

l

)

(

)

(

)

(

)

(

WB FF

b

a

b

b

b

b

abs

WB

abs

FF

abs

abs

l

l

l

l

l

l

)

(

)

(

)

(

)

(

The “MWAA model

” [D. Massabò et al., 2015] exploits two different decompositions of b

abs

,

based on:

1) The AAE of BrC (

BrC

)  <

BrC

> = 3.8 0.2

Processing the absorption coefficients measured

at 5-l, the “MWAA model” provides:

2) The relative contributions to the total

absorption coefficient (b

abs

) of

BC

FF

,

BC

WB

and

BrC

at every measured

l

SOURCES

BC and BrC spectral dependences

Samples: ≈ 300 24h PM10 samples, collected on quartz fiber filters.

The Multi-Wavelength Absorbance Analyzer

Instruments:

3) The apportionment of OC: from fossil fuels

(OC

FF

), wood burning (OC

WB

) and originated

by non combustion sources (OC

NC

)

Where:

Sampling site: Propata, Ligurian

Appennines, ~ 1000 m a.s.l.

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 C o ncen tra ti o n [m g m -3 ] OCFF OCWB OCNC

The Multi-Wavelength Absorbance Analyzer (MWAA) is a prototype

instrument realized at the Physics Department of the University of Genoa.

We developed an algorithm for the apportionment of the absorption coefficient (b

abs

) of the atmospheric aerosols:

Mean BCFF, BCWB and BrC light absorption coefficients as a function of wavelength at Propata during winter 2014

y = 1.01 x + 0.15 R² = 0.98 0% 20% 40% 60% 80% 100% 120% 0% 20% 40% 60% 80% 100% f NF x 10 0 ( 14 C) ( TC - TCFF ) / TC

D. Massabò et al., Atmospheric Environment: 108, 1-12, 2015

y = 4.88x + 0.12 R² = 0.96 0.0 0.5 1.0 1.5 2.0 2.5 0.00 0.10 0.20 0.30 0.40 0.50 OC WB (m g m -3 ) Levoglucosan (mg m-3)

The methodology has been validated against Levoglucosan and

14

C measurements:

The

split point

is operationally set at the moment in which the laser signal is back to its

starting value. EC/OC separation is based on the assumption that EC is the only light

absorbing species present on the filter.

This is no more true if BrC is present on the filter!

But we know the fraction absorbed by BrC @ 635nm (

MWAA model

)

14% 5% 4% 11% 12% 11% 5% 7% 0% 9% 7% 0% 14% 13% 15% 11% 3% 7% 8% 17% 11%14%23% 17% 22% 25% 10% 9% 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 EC (m g m -3 )

EC

Original EC Modified EC 5% 1% 1% 2% 3% 2% 2% 3% 0% 2% 2% 0% 4% 2% 4% 2% 1% 2% 1% 3% 0% 2% 3% 2% 4% 4% 2% 2% 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 OC ( mg m -3 )

OC

Original OC Modified OC

We can implement the information obtained by the optical apportionment in order to correct the starting value

of the laser. Basically we subtracted the attenuation value of the BrC to the total attenuation.

Riferimenti

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