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Pyro-convective cloud from aircraft ~ 10km (N57, W125) June 27, 2004

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High Temporal Resolution Inverse Modeling Analysis of CO Emissions from North American Boreal Fires During the Summer of 2004 Importance of Their Injection Height. - PowerPoint PPT Presentation
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Solène Turquety – AGU fall meeting, San Francisco, December 2006 High Temporal Resolution Inverse Modeling Analysis of CO Emissions from North American Boreal Fires During the Summer of 2004 Importance of Their Injection Height S. Turquety 1,2 , D. J. Jacob 1 , J. A. Logan 1 , C. L. Heald 4 , D. B. Jones 3 , R. C. Hudman 1 , F. Y. Leung 1 , R. M. Yantosca 1 , S. Wu 1 , L.K. Emmons 5 , D. P. Edwards 5 , G. W. Sachse 6 Pyro-convective cloud from aircraft ~ 10km (N57, W125) June 27, 2004 www.cpi.com/remsensing/midatm/smoke.ht ml 1 Harvard University, Cambridge, USA 2 Service d’Aéronomie, IPSL, UPMC, Paris, France 3 University of Toronto, Canada 4 University of California Berkeley, USA 5 NCAR, Boulder, USA 6 NASA Langley Research Center, Hampton, USA Uncertainty on the fire emissions (area burned, fuel consumed, etc.) Importance of injection heights more and more recognized but highly uncertain
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Solène Turquety – AGU fall meeting, San Francisco, December 2006

High Temporal Resolution Inverse Modeling Analysis of CO Emissions from North American Boreal Fires During the Summer of 2004

Importance of Their Injection Height

S. Turquety1,2, D. J. Jacob1, J. A. Logan1, C. L. Heald4, D. B. Jones3, R. C. Hudman1, F. Y. Leung1, R. M. Yantosca1, S. Wu1, L.K. Emmons5, D. P. Edwards5, G. W. Sachse6

Pyro-convective cloud from aircraft ~ 10km (N57, W125) June 27, 2004www.cpi.com/remsensing/midatm/smoke.html

1Harvard University, Cambridge, USA2Service d’Aéronomie, IPSL, UPMC, Paris, France3University of Toronto, Canada

4University of California Berkeley, USA5NCAR, Boulder, USA 6NASA Langley Research Center, Hampton, USA

• Uncertainty on the fire emissions (area burned, fuel consumed, etc.)• Importance of injection heights more and more recognized but highly uncertain

Solène Turquety – AGU fall meeting, San Francisco, December 2006

19 Tg

11 Tg

We constructed a daily area burned: •Temporal variability: daily reports from the U.S. National Interagency Fire Center•Location of the fires: MODIS hotspot detection

Fuel consumption and emission factors including the contribution from peat burning

Daily inventory of boreal fire emissions for North America in 2004(Turquety et al., submitted, JGR)

Summer of 2004: Largest fire year on record in terms of area burned in Alaska and western Canada;

Pfister et al., GRL, 2005: Inverse modeling a posteriori estimate 30 ± 5 Tg CO emitted based on MOPITT CO ~ twice their a priori estimate

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Evaluation using the MOPITT CO observations(Turquety et al., submitted, JGR)

Highlights the importance of peat burning

Strong uncertainty remain:→ Areas burned/Timing of fires? → Fuel consumption? → Impact of injection heights?

GEOS-Chem: no peat burning

GEOS-Chem: with peat burning

MOPITTModel with peatModel without peat

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Importance of high altitude injection in 2004

Average vertical distribution of boreal fires emissions in the CTM (F-Y Leung):

• 40% boundary layer• 30% FT ~ [600–400hPa]• 30% UT ~ [400–200hPa]

Variability CO emissions and max TOMS AI Alaska-Yukon [165-125W]

Several studies have shown that pyro-convective events occurred – and could explain some long-range transport events : e.g.

→ Damoah et al., 2006 : event end of June→ DeGouw et al., 2006 : event in mid-July

Peaks in TOMS AI suggest pyro-convection events: end of June, beginning of July, mid-July and mid-August

Solène Turquety – AGU fall meeting, San Francisco, December 2006

a priori sources xaa posteriori estimates

Inversion

Forward model: Observations:amodel xKy xKy obs

Inverse modeling of boreal fire emissions

GEOS-Chem CO * MOPITT AK

+

MOPITT CO – summer 2004

)(1

ˆ aaaa xKySKSKKSxx

TT

111ˆ

aSKSKS T (MOPITT – MODEL)

Gain matrix

Maximum a posteriori solution (Rodgers, 2000)

With S∑ : observation and model error Sa : a priori error K : Jacobians (∂y/ ∂x)

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Kalman Filter

Kalman Smoother

Analysis

Analysis

Analysis

update

tmodel ,y

tobs ,y

t01tt xxx ˆ...ˆˆ

Kalman smoother: observations from ‘future’ also used to update emissions

Time dependant inversion using a Kalman smoother

Initial conditions = MOPITT CO assimilation(D. Jones, U. Toronto)

Solène Turquety – AGU fall meeting, San Francisco, December 2006

t

1

1t

t

t,11tttttttt ε

x

x

x

KKKεxKy

...

...,,

Observations influenced by emissions for current day but also past emissions!

Separate contribution from different time steps in the model

Jacobian K now time dependant:

Time dependant inversion using a Kalman smoother

t1

t2,t1t2,t1 x

yK

with

t

update

t0

tmodel ,y

tobs ,y

Pt1tt xxx ˆ...ˆˆ

Fixed

Each emission time step update P times, last estimate = best estimate

Emissions during 3 days (1 timestep); P = 5 timesteps updated (5 x 3 = 15 days)

GEOS-Chem CO * MOPITT AK

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Model pulse simulations including vertical distribution of the emissions

State vector including vertical distribution:→ 3 biomass burning regions x 3 vertical regions: BL, MT, UT→ North American FF/BF, Asia, Rest of the world + chemical production

GEOS-Chem model simulation to be compared to the MOPITT observations:

background xKymodel

Decaying background : initial conditions = assimilated MOPITT CO (University of Toronto)

Emissions during 3 days (1 timestep); P = 5 timesteps updated (5 x 3 = 15 days)

Solène Turquety – AGU fall meeting, San Francisco, December 2006

t-1

t-2

Observationsy

Forward modelK x + bckgd

Contribution at t from emissions at t-2

Contribution at t from emissions at t

Contribution at t from emissions at t-1

t(3 days timestep)

BB AK-YK – Boundary layer BB AK-YK – Middle trop. BB AK-YK – Upper trop.

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Initial a priori uncertainty on the emissions Sa

• 50% on biomass burning emissions in our region of interest• 30% on emissions for the rest of the world• 20% uncertainty on chemical production1st adjustment of the emissions at a given timestep => errors uncorrelated 2nd adjustment of a given time step: Sa(t,t) = Sx(t,t-1) => introduce correlations

A priori uncertainty on the observations and model Se

• Determined using the method described by Heald et al., JGR, 2004uncertainty = observation – model

• Assume correlation length scale = 147 km

Total CO

Maximum error over the fire region, reflecting the large uncertainties ~ 30 –

50%

~ 5 – 20 % elsewhere

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Inversion of the emissions in 3 vertical regions: boundary layer (BL), middle troposphere (MT) and upper troposphere (UT)

Pyroconvective event end of June

Still update…

Sensitivity of the inversion to injection height, information seems to be available for the inversion of this parameter in parallel

A priori “vertdis”:40% BL, 30% MT, 30%UT

(preliminary results)

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Inversion of the emissions in 3 vertical regions: boundary layer (BL), middle troposphere (MT) and upper troposphere (UT)

Sensitivity of the inversion to injection height, information seems to be available for the inversion of this parameter in parallel

A priori “vertdis”:40% BL, 30% MT, 30%UT

(preliminary results)

Variability CO emissions and max TOMS AI Alaska-Yukon [165-125W]

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Large event in the beginning of August

Inversion of the emissions in 3 vertical regions: boundary layer (BL), middle troposphere (MT) and upper troposphere (UT)

(preliminary results)

Variability CO emissions and max TOMS AI Central Canada

From Alaska

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Conclusions and future directions

• Bottom-up emissions inventory estimate of 30 Tg CO, incl. 11 Tg CO from peat burning [Turquety et al., subm., 2006]• Including peat burning allows better agreement with first top-down estimates of 30 ± 5 Tg by Pfister et al. [2005] • Injection height is important for specific events – less important on CO averaged over the summer

• Injection heights have an impact on high temporal resolution top-down emissions inversions from MOPITT• Limited information on the vertical distribution in MOPITT• Information in the MOPITT transport pathways on injection height can be used to constrain this parameter

• Data could be used to specify injection height together with inventories: → TOMS AI→ POAM stratospheric aerosols (Fromm et al.)→ MISR : see poster Fok-Yan Leung A51C-0099→ Calipso lidar in space?→ Solar occultation measurements from ACE?

• Efforts currently undertaken to include a physical parameterization of injection heights in models• One focus of the POLARCAT international campaign to be held in 2008

Solène Turquety – AGU fall meeting, San Francisco, December 2006

Detection of vertical distribution over source regions and downwind with CALIPSO

MODIS fire detection20-26 July, 2006

Courtesy J. Pelon, Service d’Aéronomie

Solène Turquety – AGU fall meeting, San Francisco, December 2006

CO

C2H6

HCN

(+) Large variety of species measuredO3, H2O, H2O2, CO, CH4, C2H6, C2H2, HCN, CH3Cl, SF6, OCS, HNO3, PAN,…

(+) Very good vertical resolution

(+) Orbit scheduled sample boreal regions in July

(-) Lack coverage (-) No data at altitudes < ~6km

Solar occultation measurementsfrom the ACE/SCISAT-1 instrument:


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