1 Tim Oke and the extension-upwards of UHI-observations into the PBL Prof. Robert Bornstein Dept. of Meteorology, San Jose State University San Jose, CA,

Slides:



Advertisements
Similar presentations
AIR POLLUTION AND METEOROLOGY
Advertisements

Introduction Irina Surface layer and surface fluxes Anton
Section 2: The Planetary Boundary Layer
Stratus. Outline  Formation –Moisture trapped under inversion –Contact layer heating of fog –Fog induced stratus –Lake effect stratus/strato cu  Dissipation.
Ch 5 – Vertical Motion & Stability
Meteorological Data Issues for Class II Increment Analysis.
Session 2, Unit 3 Atmospheric Thermodynamics
Tropical Convection: A Product of Convergence. But What Drives Convergence?  ONE THEORY: CISK  Conditional Instability of the Second Kind  A Positive.
Natural Environments: The Atmosphere
A brief synopsis of Johnson and Mapes: Mesoscale Processes and Severe Convective Weather From Severe Convective Storms sections 3.3b, 3.3c.1, 3.4 By Matt.
Atmospheric Analysis Lecture 3.
Chapter 3 Mesoscale Processes and Severe Convective Weather Meteorology 515/815 San Francisco State University Spring 2006 Christopher Meherin.
Extratropical Synoptic-Scale Processes and Severe Convection John Monteverdi Doswell, C.A. III, and L.F. Bosart, 2001: Extratropical synoptic-scale processes.
Impacts from urban & rural surface modifications on meteorology and air quality in Houston: preliminary results Haider Taha Altostratus.
Mesoscale Processes and Severe Convective Weather Richard H. Johnson and Brian E. Mapes Presentation by Chris Medjber Severe Convective Storms, Meteorological.
NYC METEOROLOGY: MODELS by BOB BORNSTEIN Dept of Meteorology, SJSU for DHS/UDS Meeting EML, NYC June 2004.
Urbanized MM5 meso-met modeling for the Houston Texas ozone SIP Prof. Bob Bornstein Dept. of Meteorology San Jose State University San Jose, CA USA
Training course: boundary layer II Similarity theory: Outline Goals, Buckingham Pi Theorem and examples Surface layer (Monin Obukhov) similarity Asymptotic.
CHAPTER 4: ATMOSPHERIC TRANSPORT
COST 715 Meteorology Applied to Urban Air Pollution Problems September 98-September 2003 Problem Issues covered Successes Conclusions.
Calculation of wildfire Plume Rise Bo Yan School of Earth and Atmospheric Sciences Georgia Institute of Technology.
Observations and Models of Boundary-Layer Processes Over Complex Terrain What is the planetary boundary layer (PBL)? What are the effects of irregular.
Chris Birchfield Atmospheric Sciences, Spanish minor.
Session 4, Unit 7 Plume Rise
MESOSCALE MODELING FOR AIR QUALITY FORECASTING by ROBERT D. BORNSTEIN DEPT. OF METEOROLOGY SAN JOSE STATE UNIVERSITY SAN JOSE, CA USA
Understanding the USEPA’s AERMOD Modeling System for Environmental Managers Ashok Kumar Abhilash Vijayan Kanwar Siddharth Bhardwaj University of Toledo.
1 The Wind. 2 3 The origin of wind The earth is unevenly heated by the sun resulting in the poles receiving less energy from the sun than the equator.
Chapter 3: Air Temperature Daily temperature variations Daily temperature variations The controls of temperature The controls of temperature Air temperature.
Convective Feedback: Its Role in Climate Formation and Climate Change Igor N. Esau.
UMM5 simulations of urban-reforestation effects on Houston UHIs for ozone-SIP emission-reduction credits R. Bornstein, H. Taha, R. Balmori San Jose State.
Transport & Deposition of Air Pollutants David Gay Coordinator National Atmospheric Deposition Program University of Illinois, Champaign, IL ,
Observations and Models of Boundary-Layer Processes Over Complex Terrain What is the planetary boundary layer (PBL)? What are the effects of irregular.
1/26 APPLICATION OF THE URBAN VERSION OF MM5 FOR HOUSTON University Corporation for Atmospheric Research Sylvain Dupont Collaborators: Steve Burian, Jason.
Introduction to Cloud Dynamics We are now going to concentrate on clouds that form as a result of air flows that are tied to the clouds themselves, i.e.
Urban Induced Precipitation Changes: Implications for Regional Planning Erica Betts April 24, 2008.
Richard Rotunno National Center for Atmospheric Research, USA Fluid Dynamics for Coastal Meteorology.
Ekaterina Batchvarova, NIMH, Sofia – NATO-ATC-MTTP 1-10 August 2007 Surface exchange and boundary-layer parametrisations in MM5 and WRF and the European.
Convective Roll Effects on Sea Breeze Fronts
CITES 2005, Novosibirsk Modeling and Simulation of Global Structure of Urban Boundary Layer Kurbatskiy A. F. Institute of Theoretical and Applied Mechanics.
Urban Heat Island and Pollution
The Dryline The dryline can be defined as the near surface convergence zone between moist air flowing off the Gulf of Mexico and dry air flowing off of.
The simplifed momentum equations Height coordinatesPressure coordinates.
Application of the urbanized MM5 to the Houston-Galveston region by R. Bornstein*, H. Taha, R. Balmori, SJSU S. Dupont, J. Ching, RTP/EPA/NOAA A. Martilli,
Composition/Characterstics of the Atmosphere 80% Nitrogen, 20% Oxygen- treated as a perfect gas Lower atmosphere extends up to  50 km. Lower atmosphere.
Lecture 11 Picking up pieces from previous lectures + – result of surface force balance – scales of motion – mesoscale systems: sea breeze, land breeze.
Understanding Air Pressure
Meteorology for modeling AP Marti Blad PhD PE. Meteorology Study of Earth’s atmosphere Weather science Climatology and study of weather patterns Study.
Air Pollution Meteorology Ñ Atmospheric thermodynamics Ñ Atmospheric stability Ñ Boundary layer development Ñ Effect of meteorology on plume dispersion.
Processes in the Planetary Boundary Layer
Impacts of Meteorological Conditions Modified by Urban Expansion on Surface Ozone over Yangtz River Delta and Pearl River Delta region, China Xuemei Wang,
Chapter 9 Winds: Small scale and local systems. Scales of motion Smallest - microscale (few meters or less) Middle - Mesoscale (few to about 100 km) Large.
Page 1© Crown copyright 2006 Boundary layer mechanisms in extra-tropical cyclones Bob Beare.
Meteorology for the Soaring Pilot Joerg Stieber Canadian Advanced Soaring.
AOSC 200 Lesson 27. A Typical Day in a Pollution Episode A common severe pollution weather pattern occurs when high pressure is centered just west of.
Temperature Inversions the cause of the smoggy brown haze.
Urban Heat Island (UHI)
Understanding Air Pressure
Case study of an urban heat island in London, UK: Comparison between observations and a high resolution numerical weather prediction model Siân Lane, Janet.
Urban Heat Island (UHI)
The ability for the ocean to absorb and store energy from the sun is due to… The transparency of the water that allows the sun’s ray to penetrate deep.
The Turbulent Structure of the Urban Boundary Layer
METR March 2004 Thermodynamics IV.
AIR POLLUTION Page: 540 Figure 19.4 Haze, smoke (particulate matter), and other pollutants cover the Los Angeles skyline during the summer of 2009.
Mark A. Bourassa and Qi Shi
Understanding Air Pressure
September 9 to 13, 2013; Reading, United Kingdom
MODELING AT NEIGHBORHOOD SCALE Sylvain Dupont and Jason Ching
UNSTABLE Science Question 1: ABL Processes
Meteorology & Air Pollution Dr. Wesam Al Madhoun
Thunderstorms.
Presentation transcript:

1 Tim Oke and the extension-upwards of UHI-observations into the PBL Prof. Robert Bornstein Dept. of Meteorology, San Jose State University San Jose, CA, USA, Prof. Julian Hunt University College, London, UK Presented at the T. R. Oke Symposium AMS Annual Meeting, Phoenix AZ Jan 2009 Funding source: NSF

2 OVERVIEW URBAN CLIMATE ELEMENTS: a review URBAN CLIMATE ELEMENTS: a review TIM OKE’S (and his group) PBL-UHI work TIM OKE’S (and his group) PBL-UHI work –Observations –Explanations –Impacts on other urban-PBL climate elements Synthesis of ideas from Synthesis of ideas from –PBL observations (Oke and his group) –Analytical fluid dynamics (work of Prof. Hunt) –Urbanized meso-met models (Bornstein & many other groups)

3 uPBL CLIMATE ELEMENTS: battles between conflicting effects Monatomic effects VISIBILTITY: decreased VISIBILTITY: decreased TURBULENCE: increased (mechanical & thermal) TURBULENCE: increased (mechanical & thermal) PBL NIGHT STABILITY: neutral PBL NIGHT STABILITY: neutral FRONTS (synoptic & sea breeze): slowed FRONTS (synoptic & sea breeze): slowed More complex effects TEMP: increased (UHI) or decreased TEMP: increased (UHI) or decreased MOISTURE: increased or decreased MOISTURE: increased or decreased WIND SPEED (V): increased or decreased WIND SPEED (V): increased or decreased WIND DIRECTION: convergence or divergence WIND DIRECTION: convergence or divergence PRECIP: increased or decreased PRECIP: increased or decreased THUNDERSTORMS: triggered or split THUNDERSTORMS: triggered or split

4 PBL scales & layers (modified after Oke, 1997) UBL UCL RSL

5 uPBL sub-layers Urban mixing layer Urban mixing layer –Non-homogeneous –Non-stationary Urban SfcBL: has several sub-layers (next slide) Urban SfcBL: has several sub-layers (next slide) Urban surface: where is it in urban meso-met models: Urban surface: where is it in urban meso-met models: –ground –roughness length, z o –rooftop –displacement height, d –top of roughness sub-layer (RSL) Urban sub-surface: consists of Urban sub-surface: consists of –ground –walls –roofs

6 Integration of all surface temperatures gives ‘the’ SUHI “Surface” temperatures and ‘the’ Sfc UHI (SUHI): from Oke 2008

7 uSfcBL sub-layers Urban Canopy Layer (UCL) Urban Canopy Layer (UCL) –Between buildings (extends from 0-h) –Flow pattern is f (W/h ratio)  skimming, vortex, or isolated-obstacle flow Roughness sub-layer, RSL Roughness sub-layer, RSL –Flux-blending layer (extends from h to 3h) –M-O theory not valid, as u * (z) Inertial sub-layer (Oke’s tower obs) Inertial sub-layer (Oke’s tower obs) –Fluxes have blended (>3h) –M-O theory is valid, as u * not f(z)

8 St. Louis nocturnal windy PBL: warm near-neutral, polluted urban-plume vs. rural stable surface-inversion urban-plume Clark & McElroy (1970): rural inversion F0FF0F T T min T T max

9 or NYC nocturnal UHI-dome (Bornstein, 1968):  in calm conditions or  along cross-wind direction during windy conditions _____ uPBL N S

10 NYC AVERAGE NOCTURNAL UHI (z): note cross-over layer (UHI < 0) aloft due to RFD, mixing, and/or sinking rural air, ?? Bars = ± σ

11 AVERAGE MONTREAL NOCTURNAL UHI (z) AS A FUNCTION OF WIND SPEED: HIS LOOKING AT PROCESSES (OKE AND EAST, 1971)  CROSS OVER (W/ SLOW SPEEDS) NO CROSS-OVER  (W/ FAST SPEEDS)

12 HIS CLEAR LINKAGE OF SFC (left) & PBL (right) UHIs

13 HIS CLEAR SYNTHESES WITH THE WORK OF OTHERS

14 HIS CLEAR SYNTHESES OF UHI-EFFECTS ON OTHER URBAN PARAMETERS (more follows) T SO 2 θ

15  Urban-induced nocturnal elevated inversion-I traps home-heating emissions  Power plant plume is trapped b/t urban-induced inversions I & II  Inversion III is regional inversion  over-estimate of mixing depth Home-heating Sources Plume

16 NOCTURNAL UHI-INDUCED SFC-CONFLUENCE: otherwise-calm synoptic flow  confluence-center over urban center of Frankfurt, Germany

17 NYC TETROON-DERIVED w-VELOCITIES: Note (a) larger during unstable daytime-hours (b) Smaller during more stable nighttime-hours (c) thin, weak nocturnal urban elev-inversion layer-base stops w γ γ (trapping)

18 NYC inversion pattern several hrs after previous x-section: Note: flow hit urban upwind edge  roughness-deceleration  up-motion  inversion raised up-motion  inversion raised V 

19 NYC URBAN EFFECTS ON ρ (g/cm): NYC URBAN EFFECTS ON ρ v (g/cm 3 ): Large night UHI, ρ v -island, & RH-deficit Day Nite

20 URBAN IMPACTS ON PRECIP INITATION BY THERMODYNAMICS (at SJSU) INITATION BY THERMODYNAMICS (at SJSU) –LIFTING FROM UHI CONVERGENCE UHI CONVERGENCE THERMAL & MECHANICAL CONVECTION vs. THERMAL & MECHANICAL CONVECTION vs. –DIVERGENCE FROM BUILDING BARRIER EFFECT AEROSOL MICROPHYSICS AEROSOL MICROPHYSICS –SLOWER SECONDARY DOWNWIND ROLE –METROMEX & PROF. D. ROSENFELD (HUJI)

21 NYC splitting thunderstorm (via precip radar-echoes) Should be due to dynamics & aerosols?

22 ATLAN UHI-INITIATED STORM: OBS GOES-SATELLITE & PRECIP (UPPER) & MM5 w’s & precip (LOWER)

23 Fluid-dynamics meso-scale PBL-UHI work of J. Hunt (part 1) Uses Uses –Linearized Navier-Stokes equations –Scale arguments –Froude No. scaling –Analytical solutions Compares effects of Compares effects of –Roughness-change –Coriolis turning –UHI magnitude –Building heights –City size –Time of day

24 Fluid-dynamics meso-scale PBL UHI-work of J. Hunt (part 2) Urban-climate parameters studied Urban-climate parameters studied –Mixing-depth variation –Mean velocity fields –Thermal & mechanical turbulence –Precipitation distribution Goals: Goals: –Synthesis of three sources of information (PBL obs, fluid dynamic scale arguments, & meso-met models) –Two papers: Weather (qualitative) & QJRMS (quantitative)

25 Some important outstanding science questions What is the cause of UHI cross-over effect What is the cause of UHI cross-over effect What are the effects of radiative flux divergence from black carbon aerosols on the thermal structure of the uPBL What are the effects of radiative flux divergence from black carbon aerosols on the thermal structure of the uPBL What are the relative roles of UHI and barrier dynamics versus urban aerosols on urban precip patterns What are the relative roles of UHI and barrier dynamics versus urban aerosols on urban precip patterns What fraction of PBL flow goes around, over, and through the city as a function of stability What fraction of PBL flow goes around, over, and through the city as a function of stability How can PBL obs be made in urban areas How can PBL obs be made in urban areas How can research meso-met models be better urbanized How can research meso-met models be better urbanized How can the urban morphological data needed as input to urbanized meso-met models be obtained How can the urban morphological data needed as input to urbanized meso-met models be obtained How will urban climate effects in various climatic regions be impacted by a changing global climate How will urban climate effects in various climatic regions be impacted by a changing global climate

26 Questions?