testing the consistency of t3l2 cyclo-stationary fluxes with 13 c observations john miller 1, scott...

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Testing the consistency of T3L2 Cyclo-stationary fluxes with 13 C observations John Miller 1 , Scott Denning 2 , Neil Suits 2 , Kevin Gurney 2 , Jim White 3 and T3 Modelers 1. NOAA/CMDL 2. CSU 3. CU/INSTAAR

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Page 1: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Testing the consistency of T3L2 Cyclo-stationary fluxes

with 13C observations

John Miller1, Scott Denning2, Neil Suits2, Kevin Gurney2, Jim White3

and T3 Modelers

1. NOAA/CMDL2. CSU3. CU/INSTAAR

Page 2: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Outline

1. Comparison of simulated and observed 13C: seasonal cycles and annual mean latitudinal gradient.

2. Sensitivity tests: a)Fractionation b)Disequilibrium c)CO2 flux – Are differences in ‘1’ meaningful?

3. Shifting flux between land and sea.4. Across model differences

Page 3: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

δ13C from Samoa:the signal is in the data!

Land Source

Land Sink

Land Sink

Expected decrease due to Fossil Fuels

(Relative) Rises in δ13C indicate a land sink for carbon, decreases indicate a source.

Page 4: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Overview of Method

1. Take CO2 fluxes derived from mean seasonal cycle inversion.

2. Multiply fluxes by isotopic signatures and add fossil fuel and disequilibrium ‘iso-fluxes’

3. ‘Multiply’ iso-fluxes by response functions to get predicted isotopic ratios

4. Compare simulated δ13C to observed.

Page 5: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Source of Inputs

1. Fluxes T3L22. Discrimination SiB2(.5)

aggregated to T3 regions3. Land disequilibrium CASA model

RH

4. Ocean disequilibrium Keeling 13C of DIC, Takahashi pCO2

5. Single value for ff

Page 6: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Posterior CO2 v. ‘Observed’ --NIES model

(good…)Amplitudes

Page 7: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Posterior CO2 v. ‘Observed’(… but not everywhere)

Page 8: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Posterior CO2 v. Observed

Page 9: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Simulated and Observed δ13C

Page 10: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Simulated and Observed δ13C

Page 11: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Simulated and Observed δ13C

Page 12: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Discrimination

Page 13: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Discrimination

Page 14: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Discrimination

Page 15: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Flux Error

1.In each month, take 0.5 sigma posterior uncertainty from Temperate N. American land flux and either a) add this to the land or the ocean (subtracting the same from the complimentary region, to conserve flux.

2.This answers the question of whether the isotopic mismatch simply falls within the already determined uncertainty in the retrieved fluxes.

Page 16: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Flux Error

Page 17: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Flux Error

Page 18: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Disequilibrium Error

Page 19: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Sensitivity to Disequilibrium Error

Page 20: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

What does this tell us?

1. Shallow gradient and small seaonality.

2. Mismatches may be partially due to incorrect specification of discrimination, but not wholly.

3. Not a function of disequilibrium or flux uncertainty.

4. What’s left is the fluxes themselves! So, we can try moving around fluxes to see if we can match the data.

Page 21: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Now, shift ~2 Pg uptake from Ocean to Land during summer

Page 22: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

However…

Page 23: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

We can restore the lat. grad. by dramatically altering

disequilibrium

Page 24: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Across Model Summary

Lat. Grad. Comparison

-0.0014

-0.0012

-0.001

-0.0008

-0.0006

-0.0004

-0.0002

0

obse

rvat

ions

CS

U

GC

TM

UC

B

UC

I

JMA

M.C

CM

3

M.N

CE

P

M.M

AC

CM

2

NIE

S

NIR

E

TM

2

TM

3

Models/Obs.

per

mil

/deg

. la

t

Series1

Page 25: Testing the consistency of T3L2 Cyclo-stationary fluxes with  13 C observations John Miller 1, Scott Denning 2, Neil Suits 2, Kevin Gurney 2, Jim White

Conclusions

1. 13C observations can improve our flux determination, especially where ‘leakage’ may exist.

2. Seasonal cycle amplitude and latitudinal gradient seem to be largely independent parameters

3. This means that we can solve for both fluxes and improved estimates of disequilibrium and thus land and ocean parameters.