julien emile-geay

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Julien Emile-Geay Julien Emile-Geay with Mark Cane, Richard Seager, Amy Clement, Naomi Naik and Alexander van Geen Warren revisited : atmospheric Warren revisited : atmospheric freshwater fluxes and “Why is no freshwater fluxes and “Why is no deep water formed in the deep water formed in the North Pacific ?” North Pacific ?”

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Warren revisited : atmospheric freshwater fluxes and “Why is no deep water formed in the North Pacific ?”. Julien Emile-Geay. with Mark Cane, Richard Seager, Amy Clement, Naomi Naik and Alexander van Geen. THC. “A notable and well-known asymmetry in the deep ocean circulation - PowerPoint PPT Presentation

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Page 1: Julien Emile-Geay

Julien Emile-GeayJulien Emile-Geay

withMark Cane, Richard Seager, Amy Clement, Naomi Naik

and Alexander van Geen

Warren revisited : atmospheric freshwater fluxes and Warren revisited : atmospheric freshwater fluxes and “Why is no deep water formed in the “Why is no deep water formed in the

North Pacific ?”North Pacific ?”

Page 2: Julien Emile-Geay

THC

“A notable and well-known asymmetry in the deep ocean circulationis that deep water forms in the North Atlantic, and not at all in the North Pacific” (adapted from Bruce Warren)

Page 3: Julien Emile-Geay

What keeps deep water from sinking in the nNP ?

Why is the nNP so fresh relative to its Atlantic counterpart?

Page 4: Julien Emile-Geay

VBS,SSss

VWB,SSWBWB

Vu,SSuu

VN,SSWBWB VS,SSss

F=P-E

V’S’Eddy salt fluxes

Interior flow :VN –VS ≈ Sverdrup transportSalt transport MS= SWBVN – SsVS

Runoff

Western Boundary

flow

SWB ~ 34 psuSu = 34.6

V’S’

H=200m

A box model for the nNPA box model for the nNP(based on Warren 1983)(based on Warren 1983)

?

Page 5: Julien Emile-Geay

Conservations equations :Conservations equations :

• Freshwater budget :

R + F + Vu + Vwb = VBS + (VN −VS )

Interior flow = VN - VS

VWB is computed as a residual

• Salt budget (southward VWB) :€

SuVu+SWBVN+V'S'+W'S'=Ss[VBS+VS−VWB]

Eddy salt fluxes Outflow V0

Interior salt flux MS = SWBVN - SsVS

Subtropical inflowUpwelling

Page 6: Julien Emile-Geay

Results and sensitivity analysis

Ss =Fs

V0

≈160

4.8×10−3 = 32.93psu

Page 7: Julien Emile-Geay

Seasonal freshwater budget

Solid line :nNP

Dash-dotted :nNA

Thin solid :nNP-nNA

Why is the nNP so rainy despite its low evaporation rate?

Page 8: Julien Emile-Geay

WINTER

Moisture is pickedfrom the Warm Pooland converged into the nNP

rM (x, y) =

1

g(uq,vq) dp

1000

300

Page 9: Julien Emile-Geay

SUMMER

Most of the northwardmoisture transport is associated with the Asian Monsoon

rM (x, y) =

1

g(uq,vq) dp

1000

300

Page 10: Julien Emile-Geay

Conclusions

•Warren was essentially right : small throughflow rate and large (P-E) make the nNP so fresh• But it’s P, not E : Large atmospheric moisture transports, especially the Asian Monsoon, seem to explain this excess (in NCEP at least).

Why this is not happening in the North Atlantic : • different land/sea configuration (weaker Monsoon)• skinnier basin

Ultimately, the asymmetries of the land-sea configuration can explain THC asymmetries

Page 11: Julien Emile-Geay

Mass balance at the Southern Boundary

Page 12: Julien Emile-Geay

Warren’s box model (1983) CONFUSINGWarren’s box model (1983) CONFUSING : :

Freshwater fluxes :•F=P-E•R

+ Eddy Transports ..

Julien Emile-Geay:

Julien Emile-Geay:Julien Emile-

Geay:

Julien Emile-Geay:

Page 13: Julien Emile-Geay

VBS,SSss

VWB,SSWBWB

Vu,SSuu

VN,SSWBWB VS,SSss

F=P-E

A box model for the nNPA box model for the nNP(based on Warren 1983)(based on Warren 1983)

V’S’Eddy salt fluxes

Interior flow :VN –VS ≈ Sverdrup transportSalt transport MS= SWBVN – SsVS

Runoff

Western Boundary

flow

SWB ~ 34 psuSu = 34.6

V’S’ D =200m