1 LA on a smoggy dayLA on a clear day Optical Properties of Aerosols ENVR 416 Aerosol Technology

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  • 1 LA on a smoggy dayLA on a clear day Optical Properties of Aerosols ENVR 416 Aerosol Technology
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  • Topics Definitions Extinction Scattering Visibility 2
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  • Introduction Aerosol scattering is responsible for many atmospheric events - sunsets - halos around the sun or moon - rainbows - white (extensive scattering from the surface) and black (complete scattering where light cannot penetrate) clouds - visibility degradation from pollution Aerosol light scattering is also a powerful method used by instruments that measure aerosol size and concentration - these instruments are sensitive and do not manipulate particles 3
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  • Light Scattering Regimes D p < 0.05 m described by molecular scatteringaka Rayleigh Scattering D p > 100 m described by geometric optics (diffracted, reflected, refracted rays) 0.05 m < D p < 100 m D p on the order of , described by Mie Theory NOTE: All scattering can be derived via Mie Theory, developed by Gustav Mie in 1908 using Maxwells theory of Electromagnetic Radiation. Limiting cases such as D p > allow for simplifications to be made. 4
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  • Definitions c = speed of light = 3x10 10 cm/s = f* For visible light, = 400-700 nm m = refractive index relates the change in velocity that light experiences upon going from one medium to another (a material related property) m = c/v p = speed of light in a vaccum/speed of light in a material, p 5
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  • Index of Refraction 6
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  • 7 scattering absorption Scattering portion measured with Snells Law:
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  • Index of Refraction 8 Absorption often measured via spectrophotemtry Bulk absorption For electrically conductive material For most aerosol particles
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  • Relative Index of Refraction (m r ) 9 Used to describe a two phase system, i.e. a particle in air For air For vacuum For aerosol particles in air
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  • Intensity of Light 10 detector Incident light scattered light Light arriving at a surface:
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  • Intensity of Light 11 Light from a point source: A
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  • Size Parameter () 12 - Added to simplify light scattering equations - Makes = ratio of particle size to wavelength of radiation For d p on the order of m
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  • Electromagnetic Theory 13 Light possesses wave/particle duality we will treat it as the electric wave component of EM radiation Light can be: 1) unpolarized (sunlight) 2) parallel polarized 3) perpendicular polarized
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  • 14 Topics Definitions Extinction Scattering Visibility
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  • Extinction 15 Definition: the attenuation of light along an axis resulting from scattering and/or absorption Particles Extinction is dependent upon the chemical composition of particles as well as particle size, shape, orientation and number. Light Extinction is also dependent upon the polarization and frequency of the incident beam.
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  • Extinction 16 Mathematically, how do we quantify the results of extinction? I0I0 I Lambert-Beer Law
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  • Extinction 17 Lambert-Beer Law For a monodisperse aerosol: Extinction coefficient (L -1 ) Particle area Extinction efficiency # concentration Represents fractional loss in intensity per unit length
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  • Extinction 18 Extinction Efficiency Represents the relative ability of a particle to remove light from a beam compared with blocking or interception by the projected area of the particle Does not have to approach 1 in fact: For polydisperse aerosols:
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  • Example Problem 19 If: What is: a) Number concentration in #/m 3 b) Mass concentration in g/m 3 ? Lambert-Beer Law
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  • Example Problem 20
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  • Extinction 21 Recall: Therefore, there is no single equation to calculate for all d p
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  • Extinction 22 For d p > 4 m Extinction Paradox
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  • Extinction Paradox 23 Based on the condition that extinction must be observed at long relative distances For coffee cup 100 km (rarely observed condition) d obs >>
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  • Beers Law (Mass Concentration) 24
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  • 25 Topics Definitions Extinction Scattering Visibility
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  • Scattering 26 Responsible for optical effects caused by aerosols Basis for many aerosol measuring instruments Important for visibility and radiation balance Think of an aerosol particle as a light source with its own angular distribution of light intensity
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  • Scattering 27 Physical basis The scattering of EM radiation by any system is related to the heterogeneity of that system (the physics remains the same)
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  • Scattering 28
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  • Scattering 29 Two cases In this case, the whole particle sees the same E-field and scatters in phase d p