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Summer School Rio de Janeiro March 2009 5. MODELING MARITIME PBL. Amauri Pereira de Oliveira. Group of Micrometeorology. Topics. Micrometeorology PBL properties PBL modeling Modeling surface-biosphere interaction Modeling Maritime PBL Modeling Convective PBL. Modeling Maritime PBL.
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Summer SchoolRio de JaneiroMarch 20095. MODELING MARITIME PBL Amauri Pereira de Oliveira Group of Micrometeorology
Topics • Micrometeorology • PBL properties • PBL modeling • Modeling surface-biosphere interaction • Modeling Maritime PBL • Modeling Convective PBL
Maritime PBL • Inertial layer; • Roughness layer. Sjöblom, A. and Smedam, A.S., 2003: Vertical structure in the marine atmospheric boundary layer and its implication for the inertial dissipation method, Boundary-Layer Meteorology, 109, 1-25
What is going on beneath the ocean surface Thorpe, S.A., 2004: Recent developments in the study of ocean turbulence. Ann. Rew. Earth Planet. Science., 32, 91-102.
Air-Sea Interaction Edson et al., 1999: Coupled Marine Boundary Layers and Air-Sea Interaction Initiative: Combining Process Studies, Simulations, and Numerical Models.
Some important discrepancies Wainer, et al., 2003: Intercomparison of Heat Fluxes in the South Atlantic. Part I: The Seasonal Cycle. Journal of Climate.
Convective PBL over Cabo Frio • Cabo Frio – upwelling area • Upwelling - Stable PBL • Cold Front passage disrupt upwelling • Upwelling give place to a downwelling • Dowelling - Convective PBL
References Dourado, M., and Oliveira, A.P., 2001: Observational description of the atmospheric and oceanic boundary layers over the Atlantic Ocean. Revista Brasileira de Oceanografia,49, 49-64. Dourado, M.S. and Oliveira, A.P., 2008: A numerical investigation of the atmosphere-ocean thermal contrast over the coastal upwelling region of Cabo Frio , Brazil, Atmosfera , 21(1) ,13-34. Available at: http://www.iag.usp.br/meteo/labmicro
Cabo Frio upwelling SST AVHRR NOAA (Dutra et al. 2006, XV CBMET)
Downwelling Upwelling
downwelling upwelling
Mean equations Momentum Thermodynamic Specific Humidity
Oceanic Mixed Layer Model • The turbulent mixing is strong enough so that upper ocean is characterized by a mixed layer where the temperature does notvary in thevertical direction; • Transition layer between the mixed layer and the stratified non turbulent ocean bellow is much smaller than the mixed layer so that the vertical variation of temperature can be indicated by a temperature jump; • The energy required to sustain turbulent mixing is provided by convergence of the vertical flux of TKE.
atmosphere Mixed layer ocean Oceanic Mixed Layer Model
Oceanic Mixed Layer Modeldepth (h) and temperature jump (ΔT)
Atmospheric turbulent fluxes CH, CE and CD are transfer coefficient of sensible, latent and momentum (drag coefficient).
Radiation balance at the surface Short wave down Short wave up Broadband transmissivity Albedo
Radiation balance at the surfaceLong wave contribution Long wave up Long wave down ε = 0.98 Surface emissivity a = 0.52 and b = 0.064
MIXING LAYER MODEL CLOSURE Applying TKE equation to transition layer
MIXING LAYER MODEL CLOSURE In the interface Dimensional analysis
Stationary: • 2. Shear production, molecular dissipation and pressure term are neglected in transition layer is neglected because: MIXING LAYER MODEL CLOSURE
Mixing Layer Model Transition Layer
Thermodynamic Equation Limit 0
MIXING LAYER MODEL CLOSURE Thermal mixing Mechanical Mixing
Upwelling – Stable PBL Downwelling - Convective PBL
Upwelling – Stable PBL Downwelling - Convective PBL
Upwelling – Stable PBL Downwelling - Convective PBL
Upwelling – Stable PBL Downwelling - Convective PBL
Observations • FluTuA • Campaign May 2002 • Campaign December 2008
References Bacellar, S., Oliveira, A. P., Soares, J., and Servain, J., 2009: Assessing the diurnal evolution surface radiation balance over the Tropical Atlantic Ocean using in situ measurements carried out during the FluTuA Project. Meteorological Application.http://dx.doi.org/10.1002/met.111 Available at: http://www.iag.usp.br/meteo/labmicro/index_arquivos/Page779.htm
Surface Emissivity ε = 0.97 ε = 0.97 Surface emissivity