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Transport and scavenging of radionuclides in deep convection Romain Pilon 1,2 , Jean-Yves Grandpeix 1 1 Laboratoire de Météorologie Dynamique, CEA 2 October 25th, 2011

Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

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Page 1: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

Transport and scavenging of radionuclidesin deep convection

Romain Pilon1,2 , Jean-Yves Grandpeix1

1Laboratoire de Météorologie Dynamique, CEA2

October 25th, 2011

Page 2: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

●  What processes explain the evolution of the concentration?

●  How does convection influence the particle distribution in the atmosphere?

●  Provide diagnostics for atmospheric processes parameterized           assessment

Goal

Page 3: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Transport of tracer

Page 4: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Transport of tracer

●  Radionuclide 7Be →neutral tracer●  Half­life 53days ●  Source mainly in upper tropo lower strato

Deep convection Deposition terms

Wet scavenging, dry scavenging, radioactive decay

Emanuel mass­flux scheme

Page 5: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Parameterization of convective scavenging

Convective saturated updraft

Surface

Introduction of tracerinto the cloud

Page 6: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Surface

Entrainment Mixing

Convective saturated updraft

Parameterization of convective scavenging

Introduction of tracerinto the cloud

Page 7: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Surface

Entrainment Mixing

Convective saturated updraft

Parameterization of convective scavenging

Introduction of tracerinto the cloud

Page 8: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Surface

Detrainment

Precipitationof

condensate

Convective saturated updraft

Parameterization of convective scavenging

Entrainment Mixing

Introduction of tracerinto the cloud

Page 9: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Surface

Unsaturated downdraft

Parameterization of convective scavenging

unsaturated

Page 10: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Unsaturated downdraft

Resolving these budget equations

Parameterization of convective scavenging

Impaction term

unsaturated

Page 11: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Experimental simulation: TOGA with 7Be

Page 12: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Experimental simulation: TOGA with 7Be

Evaporation

Page 13: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Experimental simulation: TOGA with 7Be

● Precipitation● Entrainment  into the cloud

● Entrainment into the  unsaturated downdraft

Page 14: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Experimental simulation: TOGA with 7Be

Integral of concentration in the atmosphereBlack: no convective scavenging, red, with convective scavenging

Difference between the 2 curves precipitation

DEC JAN FEV

Page 15: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

TOGA with 7Be and datas 

●  Convective scavenging increases levels of concentration at the surface

●  Magnitude closer to the datas

Surface concentrationsBlack: CTBTO datas, blue: without convective scavenging, purple: with convective scavenging

Page 16: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Summary and outlook

● Process­based convective scavenging

● Tool for validation of convective scheme parameterization

● Help to understand processes in convection

● Comparison with CRM

● Model­data comparison methodology (GCM)

● Paleoclimatology (10 Be)

Page 17: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Page 18: Transport and scavenging of radionuclides in deep convection · 2011. 11. 22. · Transport and scavenging of radionuclides in deep convection Romain Pilon1,2, Jean-Yves Grandpeix1

 

Wet scavenging

with

particle size aerosol numberconcentration

drop size collisionefficiency

terminal velocityof rain drop