Cyclo-stationary inversions of 13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits,...

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Cyclo-stationary inversions of 13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers
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Transcript of Cyclo-stationary inversions of 13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits,...

Page 1: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Cyclo-stationary inversions of 13C and CO2

John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin

Gurney, Jim White & T3 Modelers

Page 2: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Outline

1. Motivation: Forward modeling with T3L2 fluxes showed 13C data could not be fit well, even considering 13C parameter uncertainty.

2. Set-up of the inversion

3. Results: What does 13C tell us, and is it different from using just CO2?

Page 3: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Model Setup

1. Cyclo-stationary (monthly mean) response functions from Transcom3-Level 2.

2. Use CO2 and 13C data to optimize:

A. Surface Fluxes (12 months x 22 regions)

B. Iso-disequilibrium (~annual x 22 regions)

C. Terrestrial fractionation (12 months x 11 regions)

Page 4: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

13C Mass Balance

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Global or 2D CalculationsF=Foce + Fland

Iterate until fluxes converge

Page 5: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Model Inputs

1. Data: 1992-1996 Detrended Monthly MeansA. 55 stations: Globalview CO2 B. 35 stations: CMDL 13C ( a la GV)

2. Model-Data Uncertainty:A. MBL N 0.5 ppm 0.05 per milB. MBL S+Tropics 0.25 0.025C. Hi-Altitude 1 0.075D. Continental 2 0.25

3. Priors and UncertaintyA. Flux: ~T3 (CASA NEP; Tak-992); 2PgC/yr, 1PgC/yrB. Disequilibrium; 5 PgC per mil/yr

C. Fractionation (SiB2): 2 per mil (4 per mil in mixed C3/C4 regions)

Page 6: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Sampling and Flux Locations

Green dots: CO2 and 13C data Black dots: only CO2 data

Page 7: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Annual Mean Disequilbrium

Page 8: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Oceanic DisequilibriumBased on measurements of pCO2 and δ13C of DIC.

Latitudinal gradient is caused by temperature dependent fractionation.

Depending on windspeed and pCO2 data set, global integral can vary by > 20 %

Annual Mean

Page 9: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Terrestrial Disequilibrium

Based on atmospheric history and CASA model of respiration. And, this assumes constant Δ over time.

Page 10: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Annual Mean Flux signatures

Page 11: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

‘Discrimination’ Map(A)

Variations dominated by C3/C4 distribution.

If not accounted for, C4 uptake looks like oceanic exchange, because of its small fractionation.

Page 12: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Fits to Data

• ‘CO2-only’ fluxes tend to underestimate 13C amplitudes in NH.

Black = ObservationsRed = Posterior (13C and CO2)Blue = Posterior (CO2 only)

Page 13: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Annual Mean FluxLand/Ocean flux = -1.5 / -1.3 GtC/yr

Page 14: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Annual Mean Flux: CO2 – 13C

Page 15: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Aggregated Seasonal Fluxes anddifferences from CO2: model mean

Page 16: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Partitioning sensitivity

-3

-2.5

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1 3 5 7 9 11Model #

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Page 17: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Annual Mean Error Reduction

Page 18: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Annual Mean Error Reductionfor Disequilibrium and Fractionation

Un

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Page 19: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Questions

1. How to propogate uncertainty in iterative inversions?

2. River fluxes affect 13C and CO2 differently – how to deal with in joint inversion?

Page 20: Cyclo-stationary inversions of  13 C and CO 2 John Miller, Scott Denning, Wouter Peters, Neil Suits, Kevin Gurney, Jim White & T3 Modelers.

Conclusions

1. 13C results imply that leakage across land/ocean boundaries exists.

2. 13C can stabilize Land/Ocean partitioning across models

3. Annual mean Land/Ocean partitioning is dependent upon disequilibrium, but seasonal patterns are not. Interannual patterns are also likely to be robust.

4. With reasonable uncertainties on 13C params, between model unc appears larger than within model uncertainty.