Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center.

Slides:



Advertisements
Similar presentations
Introduction Irina Surface layer and surface fluxes Anton
Advertisements

What’s quasi-equilibrium all about?
GABLS workshop, Stockholm, June 2007 Simple but realistic cases from Cabauw for GABLS Fred Bosveld (KNMI) with contributions from: Peter Baas Gert.
Towards Prediction of Artificial Monolayer Performance for Water Conservation Pam Pittaway & Nigel Hancock National Centre for Engineering in Agriculture.
Sandy desert Modifications of the surface radiation budget.
Meteorological Data Issues for Class II Increment Analysis.
Session 2, Unit 3 Atmospheric Thermodynamics
Boundary-layer energy transport and cumulus development over a heated mountain Bart Geerts & J. Cory Demko Joseph Zehnder.
Reading: Text, (p40-42, p49-60) Foken 2006 Key questions:
Blackbody radiation and solar radiation 1)More on Blackbody Radiation; Black body radiation 2) Magnitude of Solar radiation.
1 AirWare : R elease R5.3 beta AERMOD/AERMET DDr. Kurt Fedra Environmental Software & Services GmbH A-2352 Gumpoldskirchen AUSTRIA
Atmospheric Analysis Lecture 3.
CNRM activities during CarboEurope Regional Experiment Strategy - forecasting support - wind profiler - Ceilometer - Radiosonde soundings - Surface flux.
Craig Clements San José State University Shaorn Zhong Michigan State University Xindi Bian and Warren Heilman Northern Research Station, USDA Scott Goodrick.
5 th COPS Workshop, Hohenheim, March 2007 Turbulence and Energy Balance Network Thomas Foken Department of Micrometeorology University of Bayreuth.
University of Bayreuth Department of Micrometeorology Thomas Foken 3 rd COPS and GOP Workshop, Hohenheim, April 2006 Boundary-Layer Measurements.
Unstable Science Question 2 John Hanesiak CEOS, U. Manitoba Unstable Workshop, Edmonton, AB April 18-19, 2007.
ENAC-SSIE Laboratoire de Pollution de l'Air The Atmospheric Layers.
Ang Atmospheric Boundary Layer and Turbulence Zong-Liang Yang Department of Geological Sciences.
HWRF Model Sensitivity to Non-hydrostatic Effects Hurricane Diagnostics and Verification Workshop May 4, 2009 Katherine S. Maclay Colorado State University.
A Basic Introduction to Boundary Layer Meteorology Luke Simmons.
Boundary Layer Meteorology
Evaporative heat flux (Q e ) 51% of the heat input into the ocean is used for evaporation. Evaporation starts when the air over the ocean is unsaturated.
Review of the Boundary Layer
Peter Knippertz et al. – Continental stratus over summertime West Africa Continental Stratus over Summertime West Africa: Observations and Representation.
Priority Program SPP 1167 of the DFG Quantitative Precipitation Forecast Turbulent Fluxes and Thermal Convection in a Valley (SALVE) (1) Dept. Micrometeorology,
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association INSTITUTE OF METEOROLOGY AND CLIMATE RESEARCH,
2008 Intensive Observation Period in Arid/Semi-arid China—MAIRS Contribution to AMY Ailikun, Congbin FU International Program Office of MAIRS Chinese Academy.
Evaporation Slides prepared by Daene C. McKinney and Venkatesh Merwade
Coupled Climate Models OCEAN-ATMOSPHEREINTERACTIONS.
Evaporation What is evaporation? How is evaporation measured? How is evaporation estimated? Reading: Applied Hydrology Sections 3.5 and 3.6 With assistance.
Xin Xi. 1946: Obukhov Length, as a universal length scale for exchange processes in surface layer. 1954: Monin-Obukhov Similarity Theory, as a starting.
Understanding the USEPA’s AERMOD Modeling System for Environmental Managers Ashok Kumar Abhilash Vijayan Kanwar Siddharth Bhardwaj University of Toledo.
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association INSTITUTE OF METEOROLOGY AND CLIMATE RESEARCH,
Boundary Layer Convection Convection in the boundary layer occurs to transport heat moisture, and momentum from surface to free atmosphere Two common scenarios:
Federal Department of Home Affairs FDHA Federal Office of Meteorology and Climatology MeteoSwiss High resolution COSMO runs for dispersion applications.
50 Years of the Monin-Obukhov Similarity Theory Thomas Foken University of Bayreuth, Bayreuth, Germany.
The partitioning of the available energy at the Earth’s surface varies widely by geographic location, land surface type, exposure, soil properties, and.
Institute of Hydrology Slovak Academy of Sciences Katarína Stehlová 6 th ALPS-ADRIA SCIENTIFIC WORKSHOP 30 April - 5 May, 2007 Obervellach, Austria Assessment.
Soil moisture content at SIRTA ( m 3 /m 3 ) at different depths. SIRTA’s data has been transformed to have the same amplitude as ORCHIDEE’s simulation.
TURBULENT FLUX VARIABILITIES OVER THE ARA WATERSHED Moussa Doukouré, Sandrine Anquetin, Jean-Martial Cohard Laboratoire d’étude des Transferts en Hydrologie.
Lecture 8 Evapotranspiration (1) Evaporation Processes General Comments Physical Characteristics Free Water Surface (the simplest case) Approaches to Evaporation.
USE THESE VALUES. e(T) = e s (T Dew ) PRACTICE WITH STABILITY.
Analysis of Turbulence Development in the Morning
Large-Eddy Simulations of the Nocturnal Low-Level Jet M.A. Jiménez Universitat de les Illes Balears 4th Meso-NH user’s meeting, Toulouse April 2007.
Stable Atmosphere.
CITES 2005, Novosibirsk Modeling and Simulation of Global Structure of Urban Boundary Layer Kurbatskiy A. F. Institute of Theoretical and Applied Mechanics.
Section - 01 cont’d Lesson 2 Temperature and Heat.
OEAS 604: Introduction to Physical Oceanography Surface heat balance and flux Chapters 2,3 – Knauss Chapter 5 – Talley et al. 1.
Observed Structure of the Atmospheric Boundary Layer
MM5 studies at Wageningen University (NL) Title Jordi Vilà (Group 4) NL North sea Radar MM5 NL North sea.
A Thermal Plume Model for the Boundary Layer Convection: Representation of Cumulus Clouds C. RIO, F. HOURDIN Laboratoire de Météorologie Dynamique, CNRS,
Thomas Foken, Mathias Göckede, Matthias Mauder University of Bayreuth, Germany Department of Micrometeorology 3 nd CarboEurope-IP Integrated Project Meeting.
Evaporation What is evaporation? How is evaporation measured?
Processes in the Planetary Boundary Layer
Climate Change in the Arctic Ocean NABOS 2013 Atmospheric Boundary Layer (ABL) and Turbulence Tobias Wolf, Nansen Environmental and Remote Sensing Center.
A Case Study of Decoupling in Stratocumulus Xue Zheng MPO, RSMAS 03/26/2008.
Evaporation What is evaporation? How is evaporation measured? How is evaporation estimated? Reading for today: Applied Hydrology Sections 3.5 and 3.6 Reading.
Federal Department of Home Affairs FDHA Federal Office of Meteorology and Climatology MeteoSwiss Analyzing the TKE budget of the COSMO model for the LITFASS-2003.
A revised formulation of the COSMO surface-to-atmosphere transfer scheme Matthias Raschendorfer COSMO Offenbach 2009 Matthias Raschendorfer.
Observations of cold air pooling in a narrow mountain valley Allison Charland, Craig Clements, Daisuke Seto Department of Meteorology and Climate Science.
Meteorological Variables 1. Local right-hand Cartesian coordinate 2. Polar coordinate x y U V W O O East North Up Dynamic variable: Wind.
Boundary-Layer Meteorology and Atmospheric Dispersion
Surface Energy Budget, Part I
Lecture 8 Evapotranspiration (1)
Water Vapor Calculation
Climate Dynamics 11:670:461 Alan Robock
Session 6: Atmospheric Boundary Layer
Ming-Dah Chou Department of Atmospheric Sciences
Preliminary validation results of the prognostic 3d-TKE-scheme
Presentation transcript:

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Generation of free convection in a valley due to changes of the local circulation system Rafael Eigenmann, Thomas Foken Dept. Micrometeorology, University of Bayreuth 7 th COPS Workshop 27 th -29 th October 2008, Strasbourg

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Content Data basis of the study Local circulation system in the Kinzig valley Near-ground generation of free convection Parameters indicating free convection Characterisation of free convection event days Conclusion Future plans

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Flux calculation with the software package TK2 Footprint analysis Check for possible internal boundary layers Data basis – COPS energy balance network Station near Fussbach (UBT1ETG) in the Kinzig valley (Eigenmann, 2008; diploma thesis) Turbulence systemSodar/RASSRadiation and soil

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Kinzig valley – local circulation system Sodar measurements at COPS IOP8b: –Down-valley winds (S) at night, up-valley winds (N) during the day Wind direction [°]Wind speed [ms -1 ] Strong collapse of the horizontal wind speed in the morning hours: 6:30 – 8:50 UTC; v h < 1.5 ms -1

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Near-ground generation of free convection Detection of free convection events (FCEs) by the surface eddy-covariance system: Free convection for: –small friction velocities u * –high buoyancy fluxes Induced by the wind speed collapse during the wind direction change

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Further parameters indicating free convection (I) Ratio of the Deardorff velocity w * to the friction velocity u * : z i : visual inspection of a secondary maximum in the reflectivity profile Reflectivity [dB] (Beyrich, 1997)

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Further parameters indicating free convection (II) Buoyancy (B) and shear term (S) of the TKE equation: Wind shear : profile mast

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Circulation system regarding all COPS days Visualisation with the persistence P of wind direction: (Lugauer and Winkler, 2005) all days (n=92) event days (n=23) intermittent days (n=19) non-event days (n=37) Values between 0 and 1

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Free convection events regarding all COPS days 23 free convection event days (25%) Mean duration: 1h 24min Adjustment to the annual cycle of sunrise

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Mean diurnal courses of the classified days Above average values on ‘event days’ (Q E : ~100 Wm -2 ; Q H : ~40 Wm -2 ) Influence on temperature and moisture profiles of the ABL Density effects Support of cloud formation (fair-weather cumuli) latent heat Q E [Wm -2 ] sensible heat Q H [Wm -2 ] all days (n=92) event days (n=23) intermittent days (n=19) non-event days (n=37)

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Conclusions The local circulation system in the Kinzig valley is a powerful trigger mechanism for the generation of free convection events (FCEs) Eddy-covariance systems are able to detect FCEs with the stability parameter ζ for ζ < -1 Further parameters indicate FCEs: w * /u * and B/S FCEs may have a not negligible impact on ABL thermodynamics and its structure Contribution to the pre-convective environment of the cell at IOP8b (?)

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Future plans Follow-on project: Turbulent Fluxes and thermal convection in a valley (SALVE) Analysis of the development of free convection situations in the whole Kinzig valley atmosphere with LES modelling Supported by the flux measurements as initial field and boundary conditions Dependence on valley width and land use ? Virtual towers: attempt to close the energy balance by landscape-scale flux averaging (Prof. Th. Foken, Prof. V. Wirth, Dr. N. Kalthoff)

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Thank you for your attention !

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Further flux measurements at IOP8b Fußbach (UBT1ETG) Latent heat flux Q E Bowen ratio BoAvailable energy at the surface: net radiation Q S * minus ground heat flux Q G

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Definition of free convection Stull, R.B., Meteorology for Scientists and Engineers. 2nd edition. BROOKS/COLE, Pacific Grove, 502 pp.

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Mean diurnal courses of the classified days circulation systemtriggered by u * minimum FCEs on both ‘intermittent’ and ‘event days’ Above-average values of Q H and global radiation on ‘event days‘ stability parameter global radiation [Wm -2 ] sensible heat Q H [Wm -2 ] friction velocity u * [ms -1 ]

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Mean, standard deviation and number

Rafael Eigenmann University of Bayreuth – Department of Micrometeorology Bayreuth Center of Ecology and Environmental Research Example for the calculation of the persistence