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1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric Deposition Program Ammonia Workshop October 23, 2003 Photo from UMD Aztec, 2002

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Page 1: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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The Atmospheric Chemistry and Physics of Ammonia

Russell DickersonDept. Meteorology, The University of Maryland

Presented at the National Atmospheric Deposition Program

Ammonia WorkshopOctober 23, 2003

Photo from UMD Aztec, 2002

Page 2: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Talk Outline

I. Fundamental PropertiesImportanceReactionsAerosol formationThermodynamicsRole as ccn

II. Local Observations Observed concentrations Impact on visibility Box Model results New Detection Technique

III. Fun Stuff – if there’s time.

Page 3: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Atmospheric Ammonia, NH3

I. Fundamental Properties

Importance• Only gaseous base in the atmosphere.

• Major role in biogeochemical cycles of N.

• Produces particles & cloud condensation nuclei.• Haze/Visibility• Radiative balance; direct & indirect cooling• Stability wrt vertical mixing.• Precipitation and hydrological cycle.

• Potential source of NO and N2O.

Page 4: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Fundamental Properties, continued

Thermodynamically unstable wrt oxidation.

NH3 + 1.25O2 → NO + 1.5H2O

H°rxn = −53.93 kcal mole-1

G°rxn = −57.34 kcal mole-1

But the kinetics are slow:NH3 + OH· → NH2 + H2O

k = 1.6 x 10-13 cm3 s-1 (units: (molec cm-3)-1 s-1)Atmospheric lifetime for [OH] = 106 cm-3

τNH3 = (k[OH])-1 ≈ 6x106 s = 72 d. Compare to τH2O ≈ 10 d.

Page 5: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Fundamental Properties, continued

Gas-phase reactions:

NH3 + OH· → NH2· + H2O

NH2· + O3 → NH, NHO, NO

NH2· + NO2 → N2 or N2O (+ H2O)

Potential source of atmospheric NO and N2O in low-SO2 environments.

Last reaction involved in combustion “deNOx” operations.

Page 6: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Fundamental Properties, continued

Aqueous phase chemistry:

NH3(g) + H2O ↔ NH3·H2O(aq) ↔ NH4 + + OH−

Henry’s Law Coef. = 62 M atm-1

Would not be rained out without atmospheric acids.

Weak base: Kb = 1.8x10-5

Page 7: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Aqueous ammonium concentration as a function of pH for 1 ppb gas-phase NH3. From Seinfeld and Pandis (1998).

Page 8: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Formation of Aerosols

Nucleation – the transformation from the gaseous to condensed phase; the generation of new particles.

H2SO4/H2O system does not nucleate easily.

NH3/H2SO4/H2O system does (e.g., Coffman & Hegg, 1995).

Page 9: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Formation of aerosols, continued:

NH3(g) + H2SO4(l) → NH4HSO4(s, l) (ammonium bisulfate) NH3(g) + NH4HSO4(l) → (NH4)2SO4(s, l) (ammonium sulfate)

Ammonium sulfates are stable solids, or, at most atmospheric RH, liquids.

Deliquescence – to become liquid through the uptake of water at a specific RH ( 40% RH for ∽ NH4HSO4).

Efflorescence – the become crystalline through loss of water; literally to flower.

We can calculate the partitioning in the NH4/SO4/NO3/H2O system with a thermodynamic model; see below.

Page 10: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Cloud⇗

Page 11: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Formation of aerosols, continued

NH3(g) + HNO3(g) ↔ NH4NO3(s)

G°rxn = −22.17 kcal mole-1

[NH4NO3] Keq = ------------------ = exp (−G/RT) [NH3][HNO3]

Keq = 1.4x1016 at 25°C; = 1.2x1019 at 0°C

Solid ammonium nitrate (NH4NO3) is unstable except at high [NH3] and [HNO3] or at low temperatures. We see more NH4NO3 in the winter in East.

Page 12: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Ammonium Nitrate Equilibrium in Air = f(T)

NH3(g) + HNO3(g) ↔ NH4NO3(s)

– ln(K) = 118.87 – 24084 – 6.025ln(T) (ppb)2

1/Keq 298K = [NH3][HNO3] (ppb)2 = 41.7 ppb2

(√41.7 ≈ 6.5 ppb each)

1/Keq 273K = 4.3x10-2 ppb2

Water in the system shifts equilibrium to the right.

Page 13: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Radiative impact on stability: Aerosols reduce heating of the Earth’s surface, and can increase heating aloft. The atmosphere becomes more stable wrt vertical motions and mixing – inversions are intensified, convection (and rain) inhibited (e.g., Park et al., JGR., 2001).

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Additional Fundamental Properties

• Radiative effects of aerosols can accelerate photochemical smog formation.

• Condensed–phase chemistry tends to inhibit smog production.

• Too many ccn may decrease the average cloud droplet size and inhibit precipitation.

• Dry deposition of NH3 and HNO3 are fast; deposition of particles is slow.

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II. Local Observations

Page 16: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Annual mean visibility across the United states

(Data acquired from the IMPROVE network)

Fort Meade, MD

Page 17: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Fort Meade, MD

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Summer: Sulfate dominates.

Winter: Nitrate/carbonaceous particles play bigger roles.

Inorganic compounds ~50% (by mass)

Carbonaceous material ~40% (by mass)

Page 19: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

19• Seasonal variation of 24-hr average concentration of NOy, NO3-, and NH4

+ at FME.

Page 20: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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ISORROPIA Thermodynamic Model (Nenes, 1998; Chen 2002)

Inputs: Temperature, RH, T-SO42-, T-NO3

-, and T-NH4+

Output: HNO3, NO3-, NH3, NH4

+, HSO4-, H2O, etc.

Page 21: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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ISORROPIA Thermodynamic Model (Nenes, 1998; Chen, 2002)

Inputs: Temperature, RH, T-SO42-, T-NO3

-, and T-NH4+

Output: HNO3, NO3-, NH3, NH4

+, HSO4-, H2O, etc.

Page 22: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

22(Data acquired in July 1999)

Page 23: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

23(Water amount estimated by ISORROPIA)

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Interferometer for NH3 Detection

Schematic diagram detector based on heating of NH3 with a CO2 laser tuned to 9.22 μm and a HeNe laser interferometer (Owens et al., 1999).

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Linearity over five orders of magnitude.

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Response time (base e) of laser interferometer ∽ 1 s.

Page 27: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Page 28: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

28*Emissions from vehicles can be important in urban areas.

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Summary:• Ammonia plays a major role in the chemistry of the atmosphere.

• Major sources – agricultural.

• Major sinks – wet and dry deposition.

• Positive feedback with pollution – thermal inversions & radiative scattering.

• Multiphase chemistry

• Inhibits photochemial smog formation.

• Major role in new particle formation.

• Major component of aerosol mass.

• Thermodynamic models can work.

• Rapid, reliable measurements will put us over the top.

Page 30: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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AcknowledgementsAcknowledgementsContributing Colleagues:

Antony Chen (DRI) Bruce DoddridgeRob Levy (NASA) Jeff StehrCharles Piety Bill Ryan (PSU)Lackson Marufu Melody Avery (NASA)

Funding From:Maryland Department of the EnvironmentNC Division of Air QualityVA Department of Environmental QualityNASA-GSFCEPRI

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The End.

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MODIS: August 9, 2001MODIS: August 9, 2001

“Visible” Composite Aerosol Optical Depth at 550 nm

AOT

0.8

0.0

Phila

BaltGSFC GSFC

Balt

Phila

Highest Ozone of the Summer

Robert Levy, NASA

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Donora, PA Oct. 29, 1948

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Madonna

Harten Castle

Germany: Ruhr area

Portal figure

Sandstone

Sculptured 1702

Photographed 1908

Page 35: 1 The Atmospheric Chemistry and Physics of Ammonia Russell Dickerson Dept. Meteorology, The University of Maryland Presented at the National Atmospheric

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Madonna

Harten Castle

Germany: Ruhr area

Portal figure

Sandstone

Sculptured 1702

Photographed 1969

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