March 24, 2004EAS 4/88031 EAS 4/8803: Experimental Methods in AQ Week 11: Air Quality Management (AQM) Clean Air Act (History, Objectives, NAAQS) Emissions.

Slides:



Advertisements
Similar presentations
AIR POLLUTION AND METEOROLOGY
Advertisements

Section 2: The Planetary Boundary Layer
Atmospheric Destabilization Processes Upper Level Mixed Layer Synoptic Lifting Dynamic Destabilization Differential Advection.
Seasonal & Diurnal Temp Variations ATS351 Lecture 3.
Session 2, Unit 3 Atmospheric Thermodynamics
Transport of Air Pollutants
Richard T. McNider Atmospheric Sciences Department University of Alabama in Huntsville The Role of the Physical Atmosphere in Air.
Stability & Movement Figure 7.1 A rock, like a parcel of air, that is in stable equilibrium will return to its original position when pushed. If the rock.
Atmospheric Stability
Lecture 7-8: Energy balance and temperature (Ch 3) the diurnal cycle in net radiation, temperature and stratification the friction layer local microclimates.
Stability & Skew-T Diagrams
Textbook chapter 2, p chapter 3, p chapter 4, p Stability and Cloud Development.
Module 9 Atmospheric Stability MCEN 4131/ Preliminaries I will be gone next week, Mon-Thur Tonight is design night, 7:30ish, meet in classroom.
METO 637 Lesson 13. Air Pollution The Troposphere In the Stratosphere we had high energy photons so that oxygen atoms and ozone dominated the chemistry.
Temperature Lapse rate- decrease of temperature with height:  = - dT/dz Environmental lapse rate (  ) order 6C/km in free atmosphere  d - dry adiabatic.
THE HADLEY CIRCULATION (1735): global sea breeze HOT COLD Explains: Intertropical Convergence Zone (ITCZ) Wet tropics, dry poles Problem: does not account.
CHAPTER 4: ATMOSPHERIC TRANSPORT
Temperature, Buoyancy, and Vertical Motion Temperature, Pressure, and Density Buoyancy and Static Stability Temperature “Lapse Rates” Rising & Falling.
Review of the Boundary Layer
Observed Structure of the Atmospheric Boundary Layer Many thanks to: Nolan Atkins, Chris Bretherton, Robin Hogan.
Air Quality and Pollution The challenge to manage our atmospheric resources well.
II. Synoptic Atmospheric Destabilization Processes Elevated Mixed Layer (EML) Synoptic Lifting Dynamic Destabilization Differential Advection.
Lapse Rates and Stability of the Atmosphere
Thermodynamics, Buoyancy, and Vertical Motion
Introduction to Atmospheric Chemistry Measurements-I John Ortega National Center for Atmospheric Research Boulder, CO, USA National Center for Atmospheric.
Thermodynamics, Buoyancy, and Vertical Motion Temperature, Pressure, and Density Buoyancy and Static Stability Adiabatic “Lapse Rates” Convective Motions.
Meteorology & Air Quality Lecture-1
SEASONAL VARIABILITY OF ORGANIC MASS CONTRIBUTION TO PM2.5 WITHIN METRO ATLANTA AND FURTHER DOWNWIND K. Baumann 1, M.E. Chang 1, A.G. Russell 2, E.S. Edgerton.
Lesson 01 Atmospheric Structure n Composition, Extent & Vertical Division.
CRAZ Ozone Analysis Xin Qiu, Ph.D., ACM, EP May 3 rd, 2011.
Meteorology & Air Pollution Dr. Wesam Al Madhoun.
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.
USE THESE VALUES. e(T) = e s (T Dew ) PRACTICE WITH STABILITY.
Wildland Fire Impacts on Surface Ozone Concentrations Literature Review of the Science State-of-Art Ned Nikolov, Ph.D. Rocky Mountain Center USDA FS Rocky.
Key Terms and Concepts ELR--Environmental Lapse Rate 5°C-6.5°C/1000 m – temperature of the STILL air as you ascend through the troposphere. ALR--Adiabatic.
Transport and dispersion of air pollution
Surface Inversions, Atmospheric Stability, and Spray Drift.
Barry Baker 1, Rick Saylor 1, Pius Lee 2 1 National Oceanic and Atmospheric Administration Air Resources Laboratory Atmospheric Turbulence and Diffusion.
5.01 Heating and Cooling of the Atmosphere
Composition/Characterstics of the Atmosphere 80% Nitrogen, 20% Oxygen- treated as a perfect gas Lower atmosphere extends up to  50 km. Lower atmosphere.
Observed Structure of the Atmospheric Boundary Layer
August 1999PM Data Analysis Workbook: Characterizing PM1 Characterizing Ambient PM Concentrations and Processes What are the temporal, spatial, chemical,
A second, but different NBL case Seasonal Variation Diurnal Variation Continuous Tower-Based Ozone Measurements L.C. Patrick 1, S.J. Oltmans 2, J.C. Williams.
Measurements of Trace Gases and PM 2.5 Mass and Composition near the Ground and at 254 m agl During TexAQS 2000 and Comparison with Other Regions K. Baumann,
Meteorology for modeling AP Marti Blad PhD PE. Meteorology Study of Earth’s atmosphere Weather science Climatology and study of weather patterns Study.
Climate and Global Change Notes 17-1 Earth’s Radiation & Energy Budget Resulting Seasonal and Daily Temperature Variations Vertical Temperature Variation.
Chapter 6. Importance of Clouds  Release heat to atmosphere  Help regulate energy balance  Indicate physical processes.
The Arctic boundary layer: Characteristics and properties Steven Cavallo June 1, 2006 Boundary layer meteorology.
March 26, 2004EAS 4/88031 EAS 4/8803: Experimental Methods in AQ Week 11: Air Quality Management (AQM) Clean Air Act (History, Objectives, NAAQS) Emissions.
Atmospheric Stability Terminology I Hydrostatic Equilibrium –Balance, in the vertical, between PGF and gravity –The general state of the atmosphere –Net.
Atmospheric Stability The resistance of the atmosphere to vertical motion. Stable air resists vertical motion Unstable air encourages vertical motion.
Atmospheric Lifetime and the Range of PM2.5 Transport Background and Rationale Atmospheric Residence Time and Spatial Scales Residence Time Dependence.
Vertical Motion and Temperature Rising air expands, using energy to push outward against its environment, adiabatically cooling the air A parcel of air.
Cloud Formation  Ten Basic Types of Clouds (Genera): l High: Ci, Cs, Cc l Middle: As, Ac l Low: St, Ns, Sc l Clouds of Great Vertical Extent: Cu, Cb 
Chapter 6 Stability and Cloud Development. Stability & Cloud Development This chapter discusses: 1.Definitions and causes of stable and unstable atmospheric.
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.
5.01 Heating and Cooling of the Atmosphere
Local Wind Systems and Temperature Structure in Mountainous Terrain
Boundary-Layer Meteorology and Atmospheric Dispersion
Thermodynamics, Buoyancy, and Vertical Motion
Chapter 3 Thermodynamics.
Air Pollution and Control (Elective- I)
4. Atmospheric transport
Water Vapor Calculation
ATMOSPHERE OBJECTIVE 1 1.What are the structural components of the
Stability and Cloud Development
Fundamentals of air Pollution Engineering
Meteorology & Air Pollution Dr. Wesam Al Madhoun
K. Baumann, M.E. Chang, V. Dookwah, S. Lee, A.G. Russell
EART30351 Lecture 2.
Presentation transcript:

March 24, 2004EAS 4/88031 EAS 4/8803: Experimental Methods in AQ Week 11: Air Quality Management (AQM) Clean Air Act (History, Objectives, NAAQS) Emissions and Atmospheric Trends (Links) Principal Measurement Techniques (NOx, CO, SO 2 ) Measurement of CO (Exp 5) NDIR Method (Interferences, Stability, DL, Precision, Accuracy) Controlling O 3 and PM 2.5 Principal Measurement Techniques (O 3, PM 2.5 ) Atmospheric Transport & Photochemistry (NOx vs VOC, SOA) Ambient Measurements and Trends (World, USA, GA) Measurement of O 3 (Exp 6) UV Absorption (Interferences, Stability, DL, Precision, Accuracy)

March 24, 2004EAS 4/88032 T apered E lement O scillating M icrobalance If PM of mass  m deposit on piezoelectric quartz crystal, frequency changes by  f = K q Q t c m with sensitivity K q, aerosol mass flow Q, time t, and PM mass concentration c m

March 24, 2004EAS 4/88033 TEOM Method If PM of mass  m deposit on piezoelectric quartz crystal, frequency changes by  f = K q Q t c m with sensitivity K q, aerosol mass flow Q, time t, and PM mass concentration c m

March 24, 2004EAS 4/88034 TEOM Setup and Operation Reducing H 2 O Interference Inclusion of Nafion dryer using TEOM’s exhaust (low p, dry) as sheath flow. Filter housing T-controlled at 50 o C.

March 24, 2004EAS 4/88035 Assessing Accuracy of PM 2.5 Mass Measurements Comparison of dry TEOM averages with dehydrated Teflon samples Williams Tower is ~20 km west of LaPorte, which is close to Ship Channel 254 m agl6 m agl

March 24, 2004EAS 4/88036 High Resolution vs Integrated [PM 2.5 ] at LaPorte and Williams Tower Large [PM 2.5 ] transients (spikes) at both sites: Chemistry or transport? Transients (changes in [PM 2.5 ]) larger at WT, esp. at night. Averages of integrated samplers (8-24h) are very similar and follow a regional trend.

March 24, 2004EAS 4/88037 Adding Photochemistry (O 3 ) LP max [O 3 ] on 08/30 is more than twice WT-[O 3 ], which seems to follow a “rising tide”. Fast P(O 3 ) at LP (<200 ppb/h): high precursor emissions (Alkenes, NOx) in Ship Channel. More regional influence from BB plume on 9/5 + 9/6: joint increase in [PM 2.5 ].

March 24, 2004EAS 4/88038 Average Diurnal Differences in [O 3 ] and [PM 2.5 ] WT-O 3 levels are significantly higher at night and early mornings: Separation from nocturnal surface inversion; LP-O 3 titration. LP-O 3 higher at midday: >P(O 3 ) from precursor mix and closer sources. Trend to higher WT-[PM 2.5 ] mostly at night, similar to vertical gradients at Hendersonville, but note 20 km WT-LP distance!

March 24, 2004EAS 4/88039 Vertical Gradients of PM 2.5 Direct emissions and/or secondary formation of fine PM aloft. Free Troposphere Source for PM 2.5 ! During SOS’99, 16 June - 22 July 1999, measurements near Nashville, TN, between 4 and 42 m agl showed positive vertical gradients for % of all daytime, and % of all nighttime samples of PM 2.5 mass, SO 4 =, NO 3 -, and NH 4 + !!

March 24, 2004EAS 4/ Vertical Gradients of PM 2.5 Free Troposphere Source for PM 2.5 ! BL Dynamics Important Influence on Ground- Based AQ Monitoring !!

March 24, 2004EAS 4/ Vertical Wind Profile: Advection Horizontal Transport Near logarithmic increase of WS and uniform WD within well-mixed BL. Clockwise rotation with height near BL top to merge with more geostrophic winds. Nighttime separation of layers with different wind speeds and directions.

March 24, 2004EAS 4/ PM 2.5 Wind Roses: Seasonal Differences Across GA Indications for Regional Advective Transport? Period MAY-OCT NOV-APR Aug’99

March 24, 2004EAS 4/ …Similarity to Daytime O 3 Period MAY-OCT NOV-APR Aug’99

March 24, 2004EAS 4/ Summertime PM 2.5 – Max(O 3 ) Relationship Tighter correlation in July “Downwind” Griffin site offset to higher PM 2.5 mass. August 99 in Atlanta was hotter, dryer, more polluted with O 3 -precursor species.

March 24, 2004EAS 4/ Seasonal & Regional Comparison of PM 2.5 Composition Summer Months Regional Difference: Higher OM/OC and OC/EC at more rural site! Seasonal Difference: Lower OM/OC and (higher) OC/EC in winter. More SOA in August 99? More oxygenated POCs away from Atlanta? Winter Months

March 24, 2004EAS 4/ Atlanta JST Griffin downwind Elevated regional O 3 background reflected in regression’s intercept: higher in Aug 99! At JST higher intercept and slope during Aug ’99 (OPE= 4 vs 3): more efficient P(O 3 ). OPE in air mass arriving at Griffin is likely larger given by upper and lower limits. Lower limit assumes 1 st order loss of HNO 3 due to surface deposition at k ≈ 0.22 h -1. Air mass transitions from VOC-limited to NOx-limited regime due to Biogenic HC. High photochemical activity P(O 3 ) allows for high P(SOA): rural/urban gradient. Photochemical Activity Source – Receptor Considerations: O 3 /NOz as “OPE”

March 24, 2004EAS 4/ Photochemical Processes Leading to O 3 and PM SOA NOz An Assessment of Tropospheric Ozone Pollution, A North American Perspective, NARSTO, National Acad. Press, 2000.

March 24, 2004EAS 4/ Ozone Isopleths Area of effective VOC control (most often highly populated areas) Volatile Organic Compounds (VOC) Nitrogen Oxides (NO x ) Constant [O 3 ] Low [O 3 ] High [O 3 ] NOx control effective (areas with high biogenics)

March 24, 2004EAS 4/ SOA & O 3 Formation and Transport PM, SO 2, NO x Emissions VOC Emissions Wind Deposition Rainout O 3, HNO 3 PM NO hvhv RO 2 /HO 2 RO,OH NO 2 O2O2 O3O3 HNO 3 OH Fine PM, SOA

March 24, 2004EAS 4/ P lanetary B oundary L ayer Dynamics Comparison of PBL and Free Troposphere Characteristics PropertyPBLFT TurbulenceNear continuous over Z i.Convective clouds; sporadic in thin layers extending horizontally. FrictionLarge drag & energy dissipation.Small viscous dissipation. DispersionRapid in vertical & horizontal.Small molecular diffusion; rapid horizontally by mean wind. WindsWS log profile in surface layer.Nearly geostrophic. Vertical TransportMainly turbulence.Mean wind, cumulus-scale. Thickness100 – 3000 m, f (time/space).8 – 18 km, less variable. Diurnal oscillations over land.Slow time variations. PBL strongly influenced by Earth’s surface, responding to surface forcings within min

March 24, 2004EAS 4/ Turbulence in PBL Assuming an air parcel rises or sinks adiabatically, i.e. no energy is supplied nor removed, it expands and cools as it reaches lower ambient pressure aloft, or compresses and warms as it reaches higher pressure below. If the ambient vertical temperature profile (lapse rate) is less steep, the air parcel will continue to rise or fall once in (vertical) motion. Superadiabatic T profile (unstable layer)

March 24, 2004EAS 4/ Consequences for Dispersion/Dilution Weakly instable to neutral layer: Dispersion driven by advection (horizontal WS). Highly instable layer: Dispersion driven by thermal looping (vertical & horizontal).

March 24, 2004EAS 4/ Effects of Terrain (Friction)

March 24, 2004EAS 4/ Temperature Inversion Assuming an air parcel rises or sinks adiabatically, i.e. no energy is supplied nor removed, it expands and cools as it reaches lower ambient pressure aloft, or compresses and warms as it reaches higher pressure below. If the ambient vertical temperature profile (lapse rate) is steeper, the air parcel will return to its original position. Subadiabatic T profile (stable layer)

March 24, 2004EAS 4/ Inversion Types and Formation Elevated Surface Subsidence inversion: Large scale sinking of cold (but warming) air meets rising cooling air (thermals) under regional high pressure conditions. Frontal inversion: Warm moist air from S glides over cold dry air from N. Radiational inversion: Radiative heat loss at night from the Earth’s ground into space according to  T g 4.

March 24, 2004EAS 4/ Typical PBL Evolution in Summer Stull, R. B., 1988: An Introduction to Boundary Layer Meteorology. Kluwer Academic, 666 pp.

March 24, 2004EAS 4/ Potential Temperature (  ) Profiles …is T an air parcel at P and T would have if it were at P s (conserved for adiabatic motions, i.e., d  /dt = 0). Afternoon After sunset Before sunrise After sunrise Before noon Noon

March 24, 2004EAS 4/ PBL Winter vs Summer

March 24, 2004EAS 4/ Seasonal Differences in Diurnal Cycles of PM 2.5 Midday minimum due to BL mixing seems compensated by SOA in summer. PM 2.5 sources near Columbus drive nighttime averages in winter 2001/02. Summer stagnation with high O 3 also leads to high PM 2.5 (e.g. 2000). Annual PM 2.5 NAAQS (15  g m -3 ) sensitive to: - SOA formed under regional stagnation in summer; - Primary PM 2.5 from local sources at night in winter. WinterSummer

March 24, 2004EAS 4/ PM 2.5 Exceedances at Columbus in Oct-Nov 2001

March 24, 2004EAS 4/ PM 2.5 at Columbus in Oct-Dec 2001 Critical parameters driving [PM 2.5 ]: size of burn, distance and plume trajectory atmospheric divergence (horizontal wind speed) {vertical} boundary layer stability (T difference) BL mixing depth at night (BLH night )