update on stratocumulus simulations by the ucla agcm

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Update on stratocumulus simulations by the UCLA AGCM C. R. Mechoso, I. Richter, G. Cazes, and R. Terra University of California, Los Angeles OUTLINE 1. Sensitivity of Sc incidence to African orography 2. A comparison with similar results for South American orography 3. Aspects of PBL parameterization in AGCMs 4. Work in progress Mechoso, C. R., J. -Y. Yu and A. Arakawa, 2000: A coupled GCM pilgrimage: From climate catastrophe to ENSO simulations. General Circulation Model Development: Past, Present and Future. D. A. Randall Ed., Academic Press, 539-575

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Update on stratocumulus simulations by the UCLA AGCM. C. R. Mechoso, I. Richter, G. Cazes, and R. Terra University of California, Los Angeles OUTLINE Sensitivity of Sc incidence to African orography A comparison with similar results for South American orography - PowerPoint PPT Presentation

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Page 1: Update on stratocumulus simulations  by the UCLA AGCM

Update on stratocumulus simulations

by the UCLA AGCM

C. R. Mechoso, I. Richter, G. Cazes, and R. TerraUniversity of California, Los Angeles

OUTLINE

1. Sensitivity of Sc incidence to African orography

2. A comparison with similar results for South American orography

3. Aspects of PBL parameterization in AGCMs

4. Work in progress

Mechoso, C. R., J. -Y. Yu and A. Arakawa, 2000: A coupled GCM pilgrimage: From climate catastrophe to ENSO simulations. General Circulation Model Development: Past, Present and Future. D. A. Randall Ed., Academic Press, 539-575

Page 2: Update on stratocumulus simulations  by the UCLA AGCM
Page 3: Update on stratocumulus simulations  by the UCLA AGCM

Why Stratocumulus Matter• Stratocumulus cover a large portion of the world’s

oceans• Impact on global radiation budget is significant (e.g.

Slingo 1990, Hartmann et al. 1992)• Climate of tropical regions strongly depends on

subtropical marine stratocumulus: position of the ITCZ, SST gradients (e.g. Philander et al. 1996, Ma et al. 1996)

• AGCMs difficulties with stratocumulus lead to

large uncertainties in global warming estimates

severe problems in coupled GCMs (double ITCZ, warm SST bias, weakened trade winds etc.)

Page 4: Update on stratocumulus simulations  by the UCLA AGCM

Overall Goal of this Study

• Increase understanding of the interplay between the large-scale environment and subtropical marine boundary layer clouds concerning their seasonal cycle in different regions of the world oceans.

• A first stage of the study focuses on the role that orography plays on the flow over the eastern tropical oceans.

Page 5: Update on stratocumulus simulations  by the UCLA AGCM
Page 6: Update on stratocumulus simulations  by the UCLA AGCM

Seasonal Cycle of Stratocumulus

Peruvian and Namibian stratuspeak in October

Surface observations of the five major marine stratocumulus regions (from Klein and Hartmann, 1993)

Page 7: Update on stratocumulus simulations  by the UCLA AGCM

Model Description

• UCLA AGCM, version 7.1• Resolution: 2.5ºlon x 2ºlat x 29 levels• Harshvardhan (1987) radiation scheme• Prognostic version (Pan and Randall 1998) of the

Arakawa-Schubert (1974) cumulus parameterization• Mixed-layer PBL parameterization based on

Deardorff (1972), as designed by (Suarez et al. 1983) and revised by Li et al. (1999, 2002). The PBL top is a coordinate surface; a cloudy sublayer develops is this top is above condensation level.

• Climatological monthly-mean SSTs prescribed

Page 8: Update on stratocumulus simulations  by the UCLA AGCM

Experiment Design

• Test the impact of orography on stratocumulus by using the UCLA AGCM

• Contrast pairs of simulations:– Control: realistic orography everywhere– No-Orography: orographic surface heights set to

sea-level over the African (South American) continent

• Control is 20-year long. No-Orography runs are 3-year long.

Page 9: Update on stratocumulus simulations  by the UCLA AGCM

African Orography

Contour Interval = 500m

Page 10: Update on stratocumulus simulations  by the UCLA AGCM

Stratocumulus Incidence in Control

AGCM v7.1 2.5x2x29L

Page 11: Update on stratocumulus simulations  by the UCLA AGCM

Verification using NCEP Reanalysis

Control

NCEP

Contour Int. = 2 K

Page 12: Update on stratocumulus simulations  by the UCLA AGCM
Page 13: Update on stratocumulus simulations  by the UCLA AGCM

Impact on TOA Radiative Budget August

CI = 20 W/m2SW + LW positive

Page 14: Update on stratocumulus simulations  by the UCLA AGCM

Annual Cycle in the Namibian Stratus Region

Stratocumulus Incidence [%]

Lower Tropospheric Stability [K]

Page 15: Update on stratocumulus simulations  by the UCLA AGCM

Longitude-Height Section of TemperatureDifference Control - No-Orography

Average 20S-10SP

ress

ure

[mb]

LongitudeContour Int. = 1K

Page 16: Update on stratocumulus simulations  by the UCLA AGCM

Thermodynamic Energy Equation

1: Temperature Tendency2: Diabatic Effects3: Vertical Advection4: Horizontal Advection

1 2 3 4

Page 17: Update on stratocumulus simulations  by the UCLA AGCM

Calculation of terms in the thermodynamic equation

• Monthly accumulated value of diabatic effects is provided by the model.

• Monthly temperature tendency is provided by the instantaneous model output.

• Horizontal advection is computed off-line from monthly-mean model output.

• Vertical advection is obtained as a residual.

Page 18: Update on stratocumulus simulations  by the UCLA AGCM

Horizontal Temperature Advection at 700 mbAugust

Control

NAfO

Difference

Contour Interval = 0.5 K/day

Page 19: Update on stratocumulus simulations  by the UCLA AGCM

Annual Cycle of Thermodynamic Balance Terms700 mb Level

Diabatic Heating

Vertical Advection

Horizontal Advection

NAfO

Control

Page 20: Update on stratocumulus simulations  by the UCLA AGCM

Anti-Cyclonic CirculationWind and Temperature at 700 mb, August

Control

NAfO

Difference

Contour Interval = 0.5 KContour Interval = 2 K

Page 21: Update on stratocumulus simulations  by the UCLA AGCM

Difference Control minus NAfO900 mb

Contour Interval = 1 K

Page 22: Update on stratocumulus simulations  by the UCLA AGCM
Page 23: Update on stratocumulus simulations  by the UCLA AGCM
Page 24: Update on stratocumulus simulations  by the UCLA AGCM

Thermodynamic Balance TermsPeruvian Stratus Region

Diabatic Heating

Vertical Advection

Horizontal Advection

Control

NSAO

Page 25: Update on stratocumulus simulations  by the UCLA AGCM

Linear vs. Non-Linear Mountain Effect

(after Rodwell and Hoskins 2001)

Linear Response:

Anti-cyclone over the

mountain

Non-Linear Response:

Anti-cyclones to the west and east of the mountain

Page 26: Update on stratocumulus simulations  by the UCLA AGCM

Orographic Effects on Marine Stratocumulus

• Peruvian case (“nonlinear”)

West of the Andes, conservation of potential vorticity for parcels descending equatorwards along the isentropes results in increased static stability at lower levels.

• Namibian case (“linear”)

West of the African mountains, warm air advected polewards results in increased static stability at lower levels. The warm advection is a component of the anti-cyclonic circulation centered above the mountains.

• In both cases, mountains contribute to cold advection near the surface of the ocean.

Page 27: Update on stratocumulus simulations  by the UCLA AGCM

Seasonal Cycle of Stratus• California stratocumulus peak in the northern

summer, under the subsidence associated with the North American monsoon

• Peruvian and Namibian stratocumulus have broad peaks in the austral spring. – Continental orography seems to contribute to the

early start by increasing the temperature in the lower troposphere.

– Continental orography also seems to contribute to the late end by advection of cold air near the surface.

– Convection over the adjacent continents appears to play a minor role

Page 28: Update on stratocumulus simulations  by the UCLA AGCM
Page 29: Update on stratocumulus simulations  by the UCLA AGCM
Page 30: Update on stratocumulus simulations  by the UCLA AGCM
Page 31: Update on stratocumulus simulations  by the UCLA AGCM
Page 32: Update on stratocumulus simulations  by the UCLA AGCM
Page 33: Update on stratocumulus simulations  by the UCLA AGCM

Determination of Surface Fluxes Konor and Arakawa (2001)

Randall and Moeng et al. (1998, unpublished)

Surface flux of a quantity :Y

(FY)S = r PBL CY (ePBL)1/2 (YS - YPBL)

r PBL : Mean density of air within PBL

CY : Surface transfer coefficient of YePBL : Mean TKE within PBL

YS : Value of Y at the surface (ground)

YPBL : Mean value of Y within PBL's subcloud layer

Page 34: Update on stratocumulus simulations  by the UCLA AGCM
Page 35: Update on stratocumulus simulations  by the UCLA AGCM
Page 36: Update on stratocumulus simulations  by the UCLA AGCM

Annual Cycle of Simulated Stratocumulus (after AGCM revisions)

3/19/04

Page 37: Update on stratocumulus simulations  by the UCLA AGCM

Work in Progress

• Explore role of convection over continents on marine stratocumulus; i.e., by modifying continental convection through surface boundary conditions on land surfaces.

• Assess the sensitivity of AGCM simulations to different, yet realistic”, orographic distributions.

• Explore these sensitivities in the context of the coupled atmosphere-ocean system.

• Explore these sensitivities in the context of the PBL parameterization of PBL clouds.