Assimilating observed seasonal cycles of CO 2 to CASA model parameters

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Assimilating observed seasonal cycles of CO 2 to CASA model parameters Yumiko Nakatsuka Nikolay Kadygrov and Shamil Maksyutov Center for Global Environmental Research National Institute for Environmental Studies Japan

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Assimilating observed seasonal cycles of CO 2 to CASA model parameters. Yumiko Nakatsuka Nikolay Kadygrov and Shamil Maksyutov Center for Global Environmental Research National Institute for Environmental Studies Japan. Outline. Introduction and motivation for this study - PowerPoint PPT Presentation

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Page 1: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

Assimilating observed seasonal cycles of CO2

to CASA model parameters

Yumiko NakatsukaNikolay Kadygrov and Shamil Maksyutov

Center for Global Environmental ResearchNational Institute for Environmental Studies

Japan

Page 2: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

Outline

• Introduction and motivation for this study• Brief description of CASA model• Method of parameter optimization: general

overview• Details of the optimization method • Results• Future plan

Page 3: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

Objective

Flux of CO2 simulated with terrestrial biosphere model (e.g. CASA) = important prior information for inverse model estimation of regional CO2 fluxes based on the measurements of atmospheric CO2.

Our group’s objective is to make the best use of remotely-sensed CO2 data (GOSAT (Greenhouse gases Observing SATellite) and OCO) → Dramatically increase the spatial distributions of available CO2 observations.

Accurate simulation of seasonal cycle of CO2 exchange by terrestrial biosphere model is one of the important factors for reliable estimation of CO2 fluxes from CO2 observations.

→ Goal of this study: to optimize the model parameters of a terrestrial biosphere model (CASA) in order to provide a best fit to the observed seasonal cycles of CO2.

Page 4: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

→ Initial attempt: Optimize the maximum light use efficiency (ε) and Q10 of Carnegie-Ames-Stanford Approach (CASA) model for each biome type to the observed seasonal cycle of CO2.

Optimizing Seasonal Cycle

Page 5: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

CASA simulates NPP as a function of solar radiation limited by water and temperature stress

→ε=Maximum light use efficiency (light use efficiency when there is no water or temperature stress).

Heterotrophic respiration is a function of temperature.

Carnegie-Ames-Stanford Approach (CASA)

10

30),(

10

txT

heterotr QR

W)f(T,εIPARRGPPNPP plant

=Light Use Efficiency

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• Q10 = Increase in heterotrophic respiration for ΔT= +10 ºC.

• Larger Q10 → Rheterotr is more sensitive to changes in temp.

Carnegie-Ames-Stanford Approach (CASA)

10

30),(

10

txT

heterotr QR

W)f(T,εIPARRGPPNPP plant

=Light Use Efficiency

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EBF: evergreen broadleaf forest BSG: Broadleaf trees and shrubs (ground cover)DBF: deciduous braodleaf forest GSL: GrasslandMBNF: mixed broadleaf and needle leaf forest BSB: Broadleaf shrubs with bare soilENF: evergreen needle leaf forest TUN: TundraDNF: deciduous needle leaf forest DST: Desert

AGR: Agriculture

Biome types in CASA

EBF

DBF

MBNF

ENF

DNF

BSG

GSL

BSB

TUN

DST

AGR

A set of 2 parameters (ε and Q10) for each biome is used for optimization.

Page 8: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

CASA (non linear wrt p)

NIES Transport Model

Inverse calculation (Minimization of cost function)

NEE (1ºx 1º)dNEE/ dpi (1ºx 1º)

Cmod (2.5ºx 2.5º)dCmod/ dpi (2.5ºx 2.5º)

Output: Optimized pi’s and Cmod (liniarized approximation).

pi (11 x 2 parameters); i.e. ε and Q10 for each biome type

Outline of Parameter Optimization

Cobs(s, m)

Page 9: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

• Initially: ε=0.55 gC/ MJ and Q10=1.50 globally.

→Total global NPP=56.5 Pg/ yr

Step 1a: CASA

Figure: NPP predicted by CASA and average of 17 models used in Potsdam Intercomparison (Cramer et al. 1999)

N S

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Step 1b: CASA NEP sensitivities

•CASA NEE sensitivities approximated linear:

x ε Q10

x0 0.55 gC/ MJ 1.50

x1 0.5525 gC/MJ 1.525

x2 0.5475 gC/MJ 1.475

Table: Parameters used to calculate first approximation of CASA NEP sensitivities.

21

21

xx

)NEE(x)NEE(x

dx

dNEE

0

xx

Figure: Seasonal cycles of CASA NEP sensitivities for each biome type. Total sensitivities for northern hemisphere.

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• Fluxes: Oceanic (Takahashi et al. 2002, monthly), anthropogenic, and terrestrial (CASA, monthly); 1ºx1º

• CASA NEP sensitivities; 1ºx1º

• Resolutions of NIES99: 2.5ºx2.5º, 15 layers (vertical), every 15 minutes.

• Driven by NCEP data (1997 to 1998 for spin-up and 1999 for analysis).

Step 2: Atmospheric Transport Model (NIES99)

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Step 2: Atmospheric Transport Model (NIES99)

←Figure: Changes in global CO2 concentration at 500 mbar (in ppm) associated with a unit change in ε (left, in gC/MJ) and Q10 (right) of evergreen needle leaf forest (ENF) for the indicated month.

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• Minimize the following cost function, G(p) to reduce the mismatches between Cmod and Cobs:

Step 3: Minimization of mismatches

222

i p

0i

d

2

obs

oceanfossilCASAobs )σ

pp(

σ

)ff)((fT̂(d)C)G(

pp

22

i p

0i

d

222

ii

iCASAioceanfossil0CASAobs

σ

pp]

dp

)(pdfT̂p)ff)((fT̂[(d)C

)G(obs

p

p

approximate Cmod

Exact Cmod

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EBF

DBF

MBNF

ENF

DNF

BSG

GSL

BSB

TUN

DST

AGR

Step 3: Minimization of mismatches

-Data from GLOBALVIEW 2006 and a network of stations operated by NIES are used.-No observations from southern hemisphere: NIES99 has a known problem with seasonal cycle of CO2 in Southern hemisphere.-Parameter optimizations were performed with and without data from Siberian CO2-observing stations.-Results of iterative calculation are presented for the case when all the data points are considered.

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Result: Parameter Optimizations

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ε, gC/ MJ

Map of optimized ε

1. Generally, vegetation in high latitude is known to have higher ε. → This trend is better seen with the results obtained with Siberian data (especially for tundra and deciduous needle leaf forest).

2. Biomes near equator have smaller ε → Reduced NPP

Without Siberian data

With Siberian data

N S

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Result: Uncertainty Reductions

prior x,

post x,x σ

σ1R

-Uncertainties of posterior parameters were reduced particularly well for ENF (evergreen needle leaf forest) and AGR (agriculture)- Biome types with suspicious (i.e. unreasonably low) ε’s (e.g. EBF, BSB, and DST) show very low reductions of uncertainties.

Biome Type

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Result: Improved Uncertainty ReductionsE

εE

Q1

0

(noSib)R

(Sib)RE

x

xx

Ex: the enhancement of uncertainty reduction due to the use of data from Siberian stations in the optimization:

Deciduous broad leaf forest (DBF), deciduous needle leaf forest (DNF) and Tundra (TUN): particularly good reductions of uncertainty

Page 19: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

EBF: evergreen broadleaf forest BSG: Broadleaf trees and shrubs (ground cover)DBF: deciduous braodleaf forest GSL: GrasslandMBNF: mixed broadleaf and needle leaf forest BSB: Broadleaf shrubs with bare soilENF: evergreen needle leaf forest TUN: TundraDNF: deciduous needle leaf forest DST: Desert

AGR: Agriculture

Biome types in CASA

EBF

DBF

MBNF

ENF

DNF

BSG

GSL

BSB

TUN

DST

AGR

Page 20: Assimilating observed seasonal cycles of CO 2  to CASA model parameters

CASA (non linear wrt p)

NIES Transport Model

Inverse calculation (Minimization of cost function)

NEE (1ºx 1º)dNEE/ dpi (1ºx 1º)

Cmod (2.5ºx 2.5º)dCmod/ dpi (2.5ºx 2.5º)

Output: Optimized pi’s and Cmod (liniarized approximation).

pi (11 x 2 parameters); i.e. ε and Q10 for each biome type

Outline of Parameter Optimization

Cobs(s, m)

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Effects of Iteration on Parameters

-Q10 and ε of mixed broadleaf and needle leaf forest (MBNF) are fluctuating most significantly. -Q10 and ε of AGR are also fluctuating by quite a bit.

Q10 and ε of a same biome have same trend.

- dNEP/dε and dNEP/dQ10 have opposite trend

- Possible to achieve similar Cmod with two different sets of Q10 and ε when constraints on parameters by observations are insufficient.

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Results: Iteration

- Q10 of MBNF was fixed at the value obtained by the 1st iteration.

→ Amplitudes of oscillation of ε of MBNF is decreased but not completely stabilized.

→ Correlation with other biomes also possible. - E.g. the amplitude of oscillation of Q10 of AGR dramatically reduced.

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0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1

M(Prior)

M(P

oste

rior

)

3rd iteration, no parameters constrained

3rd iteration, Q10 of MBNF constraine

reference line (slope=1)

212

m obs

modelobspost/prior ]

(J)σ

J)(m,CJ)(m,C[

12

1(J)M

Results: Effects on the misfit of seasonal cycle of CO2

Mprior>0.5→better match with Cobs after optimization.Mprior<0.5

→No dramatic reductions.

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Cases Total NPP

Original CASA 56.5 Gt/ yr

Without iteration 43.53 Gt/yr

After 3 inversions

(no parameters constrained)

51.75 Gt/yr

After 3 inversions (Q10 of MBNF constrained)

54.23 Gt/yr

Effects of Iteration on annual NPP

→ This method is not applicable globally at this point…- More data (especially from BSG (broadleaf trees with shrubs on the ground cover) might help.

N S

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Conclusions and future work

Conclusions Maximum light use efficiency (ε) and Q10 of CASA were optimized for each biome using observed seasonal cycles of CO2. Addition of Siberian data enhanced the reduction of uncertainty of the optimized parameters. The observed latitudinal gradient of ε was obtained. Optimization is not working near the equator. The method is quite general and can be applied to other biosphere and transport models very easily.

Future works and questions Does the oscillation stop if I keep the iteration? Try using different transport model (e.g. NICAM). It will be interesting to optimize other biospheric models.

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Acknowledgement

Shamil Maksyutov (CGER, NIES) Nikolay Kadygrov (CGER, NIES)

Toshinobu Machida (CGER, NIES) Kou Shimoyama (now at Institute of Low Temperature Science at Hokkaido University)