Uncertainties in Water vapor:Uncertainties in Water vapor: … · 2009-09-28 · Uncertainties in...

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Uncertainties in Water vapor: Uncertainties in Water vapor: Budgets in two versions of CAM (Track 1 and Track 5) C O Cécile Hannay, Dave Williamson, Jerry Olson, Rich Neale, Sungsu Park, Phil Rasch *, Andrew Gettelman and Hugh Morrisson. National Center for Atmospheric Research, Boulder *Pacific Northwest National Laboratory, Richland Climate Feedback workshop, Keck Inst

Transcript of Uncertainties in Water vapor:Uncertainties in Water vapor: … · 2009-09-28 · Uncertainties in...

Page 1: Uncertainties in Water vapor:Uncertainties in Water vapor: … · 2009-09-28 · Uncertainties in Water vapor:Uncertainties in Water vapor: Budgets in two versions of CAM (()Track

Uncertainties in Water vapor:Uncertainties in Water vapor:Budgets in two versions of CAM(Track 1 and Track 5)( )

C OCécile Hannay, Dave Williamson, Jerry Olson, Rich Neale, Sungsu Park, Phil Rasch*,

Andrew Gettelman and Hugh Morrisson.

National Center for Atmospheric Research, Boulder*Pacific Northwest National Laboratory, Richland

Climate Feedback workshop, Keck Inst

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What are Track 1 and Track 5 ?

• Track 1 = cam3.5.1- Deep convection: Neale-Richter (2008)

- Microphysics: Rasch-Kristjansson (1998)

- Boundary layer: Holtslag-Boville (1993)

- Shallow convection: Hack (1993)

- Bulk Aerosol Model (BAM, Barth, Rasch, Mahowald … 2000-2009)

- Radiation: CAMRT (Ramanathan, Kiehl, Collins,…1970s-2006)

T k 5 4• Track 5 = cam4- Deep convection: Neale-Ritcher (2008)

- Microphysics: Morrison and Gettelman (2008)p y ( )

- Boundary layer: Bretherton and Park (2009)

- Shallow convection: Park and Bretherton (2009)

M h i P k R h B th t (2009)-Macrophysics: Park, Rasch, Bretherton (2009)

- Modal Aerosol Model (MAM): Ghan and Liu

- Radiation: RRTMG: Iacono et al (2008)

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Water vapor biases

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Clear Sky OLR

Model values too lowModel values too lowPartly explained by

Emissions above top of modelmodelDifferences in Sampling methodology btw models and CERESToo much water vapor

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Motivation

• Analysis of the budget for temperature, moisture and condensate

• Climate runs:- understand the balance that controls the climate

• Forecast runs:- understand how we attain this balance

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Water vapor budget

∂q∂t

= −V •∇q −ω∂q∂p

+ Qphysics

Physics tendencies

∂t ∂pAdvective tendencies

Qpbl + Qdeep convection+ Qshallow convection + Qmacro+micro

Convective mass flux

Shallow convection Evap & Prod of Evaporationflux

Evaporation convective

precipitation

convection tendency

Evaporation

Evap & Prod of condensate

Evaporation falling

precipitation

Evaporation ofprecipitationconvective

precipitationEvaporation of

sedimenting cloud water

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Global annual means: q profiles and tendencies

Moisture tendenciesMoisture profile

− Total− Advection− Physics

Track 1 = plainTrack 5 = dash− ERA40

− JRA25− Track 1 Track 1− Track 5

MoisteningDrying

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Global annual mean: physics tendencies break-up

Track 1 Track 5Drying of upper troposphere- by Hack in Track 1- by microphysics in Track 5

− PBL− Micro+Macro− Deep− Shallow

In Track 1: MoisteningMoistening by deep convection around 500 mb

Shallow convection is stronger in Track 5

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Budget terms in various regimes

•Stratocumulus•Transition•ITCZITCZ•Bay of Bengal•Storm Tracks•Arctic•Continental US•Tropical land

http // cgd car ed /cms/hanna /internal/cam4 de /b dgets/t1 t5/B dget t1 t5 htmlhttp // cgd car ed /cms/hanna /internal/cam4 de /b dgets/t1 t5/B dget t1 t5 htmlhttp://www.cgd.ucar.edu/cms/hannay/internal/cam4_dev/budgets/t1_t5/Budget_t1_t5.htmlhttp://www.cgd.ucar.edu/cms/hannay/internal/cam4_dev/budgets/t1_t5/Budget_t1_t5.html

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Stratocumulus

Track 1 Track 5

− PBL− Micro+Macro− Deep

Shallow− Shallow

Shallow convection is stronger in Track 1

PBL moves moisture higher in the atmosphere

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Transition region

Track 1 Track 5

− PBL− Micro+Macro− Deep

Shallow− Shallow

Shallow convection is stronger in Track 5Deep convection is

stronger in Track 1

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Conclusion and future work

• Budgets help to understand the balance that controls the climate

• Water vapor tendencies are very different in Track 1 and 5• Water vapor tendencies are very different in Track 1 and 5, even when the states in the two tracks are similar.

A major difference is in the shallow convective tendencies, j ,which are globally stronger in Track 5 than Track 1

The drying of the upper troposphere is driven by different processes:- Track1: Hack convection scheme (unrealistic)- Track5: macro+micro (reflects new ice microphysics)

In the stratocumulus regions, there is an unrealistically large contribution from the shallow convection scheme in Track 1

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Future work

Next , we will look at :the temperature, liquid and ice budgets forecast runs (CAPT framework):

understand how we attain this balanceallows direct comparison of the parameterized variables (e.g. p p ( gclouds) with observations from field campaigns

How do we use observations to help us understand the balances in the real world for these regimes, and achieve g ,similar balance in models?•