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ASTEX case ASTEX case

ASTEX case - PowerPoint Presentation

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ASTEX case - PPT Presentation

Gunilla Svensson Department of Meteorology and the Bert Bolin Centre for Climate Research Stockholm University Sweden Airmass tracked by ballons and forecasts same airmass revisited with research aircraft ID: 574834

gcss svensson drizzle euclipse svensson gcss euclipse drizzle meeting cloud september 2010 astex experiment 2000 1st lagrangian vertical scale

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Slide1

ASTEX case

Gunilla Svensson

Department of Meteorology and the Bert Bolin Centre for Climate Research

Stockholm University, Sweden

Slide2

Airmass

tracked by ballons and forecasts – same airmass revisited with research aircraftSlide3

ASTEX 1

st Lagrangian experiment

EUCLIPSE/GCSS Meeting, 29-30 September 2010

Svensson et al., 2000Slide4

ASTEX 1

st Lagrangian experiment

EUCLIPSE/GCSS Meeting, 29-30 September 2010

Svensson et al., 2000Slide5

ASTEX 1

st Lagrangian experiment

1-D version of the MIUU

mesoscale

model

Hydrostatic pressure

Prescribed background flow (

geostrophic

wind)

Surface fluxes (

Fairall

et al, surface layer similarity and roughness sub-layer treatment)

Second-order turbulence closure (Mellor-Yamada type with prognostic TKE)Subgrid-scale condesationShort and long-wave radiation (Fu&Liou, delta four-stream and correlated k-distribution)A simplified algorithm for prognostic drizzle water conversion of cloud water to drizzle collection of cloud drops by raindropsfall-out of rain dropsevaporation of rain drops in sub-saturated air

EUCLIPSE/GCSS Meeting, 29-30 September 2010

Svensson et al., 2000Slide6

A sub-grid scale cloud scheme in this framework:

*

(T, q)

Temperature

Specific humidity

q

sSlide7

Model resultsSlide8
Slide9
Slide10
Slide11
Slide12

Latent heat flux and drizzle rate Slide13

SST or subsidence driving the change from Sc to Cu?

Drizzle only a few mm per day does it matter?Subsidence very small vertical motions, is it important?

In a model it is possible to pick these

pieces

apart

never possible in real life

Sensitivity experimentsSlide14
Slide15
Slide16

Z

cloud-top

LWP

Albedo

Drizzle

Z

cloud-base

Sensitivity experiments

TKESlide17

Vertical velocity at PBL top

HIRLAM simulationEUCLIPSE/GCSS Meeting, 29-30 September 2010

Sigg and Svensson, 2004

Oscillations are due to inertia-gravity waves that propagate from the non-elliptic areas where gradient-wind balance cannot be maintained.Slide18

Synoptic-scale divergence

Filtered vertical velocities removing scales smaller than 15h

South

North

EUCLIPSE/GCSS Meeting, 29-30 September 2010

Sigg and Svensson, 2004Slide19

END