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Illumination Independent Aerosol Optical Properties Extinction • Scattering • Absorption Volume scattering function (phase) Transmittance

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Page 1: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Illumination Independent Aerosol Optical Properties

Extinction• Scattering• Absorption

Volume scattering function (phase) Transmittance

Page 2: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

The extinction coefficient is made up of

particle and gas scattering and absorption:

where s, a, g, and p refer to scattering, absorption, gases, and particles, respectively.

ext sg ag sp apb = b +b +b +b

Extinction =

Page 3: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Components of Scattering and Extinction

Page 4: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Animations of scattering and absorption

Page 5: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

One Approximation for Estimating bext

].[10

]SO

]SO

344

344

lacclacf)[SOIL](e +(RH)[OMC]f)(e +

]NO(RH)[NH)f(e +iated(RH)[Ammon)f(e

)[SOIL](e +(RH)[OMC]f)(e +

]NO(RH)[NH)f(e +iated(RH)[Ammon)f(e = b

soilcocmocmc

nncssc

soilfocmocmf

nnfssfext

Page 6: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

(D)d(D)n),m(QD4

=B iie2

o

iext,

(x)dx)x,,( fmE=B iie

-

iext,

where Ee is mass extinction efficiency, f i(x) is the aerosol mass distribution dm/dx of the ith species, x=ln[D/Do], and λ is the wavelength.

Extinction as Function of Size

Page 7: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

m =B iiiext,

(x)dx)x,,( fmE=iie

o

i

where

m =B i i

iext

and for multiple species

Externally Mixed Model

Page 8: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Scattering Efficiency (Q)

Page 9: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Single Particle Efficiency

Page 10: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Particle Size Distribution

Page 11: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Scattering Efficiency as Function of Size

Page 12: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Carbon Extinction Efficiency

Page 13: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Phase Function for Soil and Sulfate

Page 14: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Phase Function for Carbon

Page 15: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Forward and Backward Scattering

Page 16: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Pollutant Species

Page 17: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Primary vs. Secondary Particles and Gases (Pollutants)

Primary particles and gases are those emitted into the atmosphere directly from some source.

Secondary particles and gases are formed in the atmosphere by chemical reactions, by condensation growth, and/or by coagulation.

Page 18: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance
Page 19: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Particle Size Distribution

Page 20: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Sources of Primary Particles

Anthropogenic Wind Blown Dust

Roads, Over Grazing, Farming practices, Mining

Biomass BurningLand Clearing Practices

Emissions from fossil fuel combustionFly Ash Condensation of Hot Vapors

Naturally Occurring Wind Blown Dust

Deserts

Volcanoes Fires Plant Particles

(pollen)

Sea Salt Spray(NaCl)

Page 21: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Sources of Primary Gases Important to Secondary Particle Formation

Compound Anthropogenic Naturally Occurring

SO2 Fossil-FuelSmelters

Oil Refining

Volcanoes 

NOxFossil-Fuel Combustion

Mobil SourcesSoil Release (Fertilizer)

Soil ReleaseLightning

NH3 Farm Animals Wild AnimalsVegetation

Ocean Volatile

OrganicsMobile Sources Vegetation

Page 22: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance
Page 23: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Hygroscopic Aerosols

Water uptake by particles in the atmosphere Aerosol particles grow and scatter more light Deliquescence - the RH value at which the

crystal begins to absorb water and becomes a solution droplet

Hysteresis - water is retained on the particle at RH values lower than predicted by equilibrium

Page 24: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Growth of Sulfate

Page 25: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Hygroscopic Growth of Particles

Page 26: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Ammonium Sulfate D/Do Curves

Page 27: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Two Measured f(RH) Curves and Theoretical Estimated

Page 28: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

F(rh) for Grand Canyon

Page 29: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Estimated f(rh) for Sulfate and Organics

] [ ...... ] [ ] [ ) (2 1 ,Species Other a OMC a SULFATE a a RH bn o water scat

Page 30: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Internally Mixed Aerosol

m B

m FM

i i

iext

i

i

however,

Page 31: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Mass Removal Issues

Page 32: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

From previous equations, it is apparent that changes in visibility that correspond to changes in aerosol species concentrations can be expressed by forming the derivative τr/Ci, where Ci refers to the concentration of

particulate species i, and that this derivative will have terms containing the derivative bext/Ci. Therefore, define partial scattering

efficiency as:

Partial Scattering Efficiency

)C/b(=e etc ,ciextp j

Page 33: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Extinction for External and Internal Mixture

Page 34: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

D/Do Curves for Partial Scattering Calculation

Page 35: Illumination Independent Aerosol Optical Properties n Extinction Scattering Absorption n Volume scattering function (phase) n Transmittance

Partial Scattering Efficiency for External and Internally Mixed Aerosols