Radiative Transfer in the Atmosphere

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Radiative Transfer in the Atmosphere. Lectures in Benevento June 2007 Paul Menzel UW/CIMSS/AOS. Using wavelengths c 2 / λ T Planck’s Law B( λ ,T) = c 1 / λ 5 / [e -1] (mW/m 2 /ster/ c m) where λ = wavelengths in cm - PowerPoint PPT Presentation

Text of Radiative Transfer in the Atmosphere

  • Radiative Transfer in the AtmosphereLectures in Benevento June 2007 Paul Menzel UW/CIMSS/AOS

  • Using wavelengths c2/TPlancks Law B(,T) = c1 / 5 / [e -1] (mW/m2/ster/cm) where = wavelengths in cmT = temperature of emitting surface (deg K)c1 = 1.191044 x 10-5 (mW/m2/ster/cm-4)c2 = 1.438769 (cm deg K)

    Wien's Law dB(max,T) / d = 0 where (max) = .2897/Tindicates peak of Planck function curve shifts to shorter wavelengths (greater wavenumbers) with temperature increase. Note B(max,T) ~ T5. Stefan-Boltzmann Law E = B(,T) d = T4, where = 5.67 x 10-8 W/m2/deg4. ostates that irradiance of a black body (area under Planck curve) is proportional to T4 .

    Brightness Temperature c 1T = c2 / [ ln( _____ + 1)] is determined by inverting Planck function 5B

  • Spectral Distribution of Energy Radiated from Blackbodies at Various Temperatures

  • 2

    1B (, T) / B (, 273K) 250 300 Temperature (K)4m6.7m10m15mmicrowaveTemperature Sensitivity of B(,T) for typical earth scene temperatures

  • Spectral Characteristics of Energy Sources and Sensing Systems

  • Normalized black body spectra representative of the sun (left) and earth (right), plotted on a logarithmic wavelength scale. The ordinate is multiplied by wavelength so that the area under the curves is proportional to irradiance.

  • Relevant Material in Applications of Meteorological Satellites

    CHAPTER 2 - NATURE OF RADIATION 2.1 Remote Sensing of Radiation2-12.2 Basic Units2-12.3 Definitions of Radiation 2-22.5Related Derivations2-5

    CHAPTER 3 - ABSORPTION, EMISSION, REFLECTION, AND SCATTERING 3.1Absorption and Emission3-13.2Conservation of Energy3-13.3Planetary Albedo3-23.4Selective Absorption and Emission3-23.7Summary of Interactions between Radiation and Matter3-63.8Beer's Law and Schwarzchild's Equation3-73.9 Atmospheric Scattering3-93.10 The Solar Spectrum3-113.11Composition of the Earth's Atmosphere3-113.12 Atmospheric Absorption and Emission of Solar Radiation3-113.13 Atmospheric Absorption and Emission of Thermal Radiation3-123.14 Atmospheric Absorption Bands in the IR Spectrum3-133.15 Atmospheric Absorption Bands in the Microwave Spectrum3-143.16 Remote Sensing Regions3-14

    CHAPTER 5 - THE RADIATIVE TRANSFER EQUATION (RTE) 5.1 Derivation of RTE5-15.10Microwave Form of RTE5-28

  • Emission, Absorption, Reflection, and Scattering

    Blackbody radiation B represents the upper limit to the amount of radiation that a real substance may emit at a given temperature for a given wavelength.

    Emissivity is defined as the fraction of emitted radiation R to Blackbody radiation,

    = R /B .

    In a medium at thermal equilibrium, what is absorbed is emitted (what goes in comes out) so a = . Thus, materials which are strong absorbers at a given wavelength are also strong emitters at that wavelength; similarly weak absorbers are weak emitters.

    If a, r, and represent the fractional absorption, reflectance, and transmittance, respectively, then conservation of energy says

    a + r + = 1 .

    For a blackbody a = 1, it follows that r = 0 and = 0 for blackbody radiation. Also, for a perfect window = 1, a = 0 and r = 0. For any opaque surface = 0, so radiation is either absorbed or reflected a + r = 1.

    At any wavelength, strong reflectors are weak absorbers (i.e., snow at visible wavelengths), and weak reflectors are strong absorbers (i.e., asphalt at visible wavelengths).

  • Planetary Albedo

    Planetary albedo is defined as the fraction of the total incident solar irradiance, S, that is reflected back into space. Radiation balance then requires that the absorbed solar irradiance is given by

    E = (1 - A) S/4.

    The factor of one-fourth arises because the cross sectional area of the earth disc to solar radiation, r2, is one-fourth the earth radiating surface, 4r2. Thus recalling that S = 1380 Wm-2, if the earth albedo is 30 percent, then E = 241 Wm-2.

  • Selective Absorption and Transmission

    Assume that the earth behaves like a blackbody and that the atmosphere has an absorptivity aS for incoming solar radiation and aL for outgoing longwave radiation. Let Ya be the irradiance emitted by the atmosphere (both upward and downward); Ys the irradiance emitted from the earth's surface; and E the solar irradiance absorbed by the earth-atmosphere system. Then, radiative equilibrium requiresE - (1-aL) Ys - Ya = 0 , at the top of the atmosphere,(1-aS) E - Ys + Ya = 0 , at the surface.

    Solving yields

    (2-aS) Ys = E , and (2-aL)

    (2-aL) - (1-aL)(2-aS) Ya = E . (2-aL)

    Since aL > aS, the irradiance and hence the radiative equilibrium temperature at the earth surface is increased by the presence of the atmosphere. With aL = .8 and aS = .1 and E = 241 Wm-2, Stefans Law yields a blackbody temperature at the surface of 286 K, in contrast to the 255 K it would be if the atmospheric absorptance was independent of wavelength (aS = aL). The atmospheric gray body temperature in this example turns out to be 245 K.

  • E (1-al) Ys Ya top of the atmosphere

    (1-as) E Ys Ya earth surface.

    Incoming Outgoing IR solar (2-aS) Ys = E = Ts4 (2-aL)

  • Expanding on the previous example, let the atmosphere be represented by two layers and let us compute the vertical profile of radiative equilibrium temperature. For simplicity in our two layer atmosphere, let aS = 0 and aL = a = .5, u indicate upper layer, l indicate lower layer, and s denote the earth surface. Schematically we have:

    E (1-a)2Ys (1-a)Yl Yu top of the atmosphere

    E (1-a)Ys Yl Yu middle of the atmosphere

    E Ys Yl (1-a)Yu earth surface.

    Radiative equilibrium at each surface requires

    E = .25 Ys + .5 Yl + Yu ,E = .5 Ys + Yl - Yu ,E = Ys - Yl - .5 Yu .

    Solving yields Ys = 1.6 E, Yl = .5 E and Yu = .33 E. The radiative equilibrium temperatures (blackbody at the surface and gray body in the atmosphere) are readily computed.

    Ts = [1.6E / ]1/4 = 287 K ,Tl = [0.5E / 0.5]1/4 = 255 K ,Tu = [0.33E / 0.5]1/4 = 231 K .

    Thus, a crude temperature profile emerges for this simple two-layer model of the atmosphere.

  • Transmittance

    Transmission through an absorbing medium for a given wavelength is governed by the number of intervening absorbing molecules (path length u) and their absorbing power (k) at that wavelength. Beers law indicates that transmittance decays exponentially with increasing path length

    - k u (z) (z ) = e

    where the path length is given by u (z) = dz . z

    k u is a measure of the cumulative depletion that the beam of radiation has experienced as a result of its passage through the layer and is often called the optical depth .

    Realizing that the hydrostatic equation implies g dz = - q dp

    where q is the mixing ratio and is the density of the atmosphere, then

    p - k u (p)u (p) = q g-1 dp and (p o ) = e. o

  • Spectral Characteristics of Atmospheric Transmission and Sensing Systems

  • Relative Effects of Radiative Processes

  • 0.010.11.010.0There are 3 modes :

    - nucleation: radius is between 0.002 and 0.05 mm. They result from combustion processes, photo-chemical reactions, etc.

    - accumulation: radius is between 0.05 mm and 0.5 mm. Coagulation processes.

    - coarse: larger than 1 mm. From mechanical processes like aeolian erosion.

    fine particles (nucleation and accumulation) result from anthropogenic activities, coarse particles come from natural processes.

    Aerosol Size Distribution

  • Scattering of early morning sun light from haze

  • Measurements in the Solar Reflected Spectrum across the region covered by AVIRIS

  • AVIRIS Movie #1AVIRIS Image - Linden CA 20-Aug-1992224 Spectral Bands: 0.4 - 2.5 mmPixel: 20m x 20m Scene: 10km x 10km

  • AVIRIS Movie #2AVIRIS Image - Porto Nacional, Brazil20-Aug-1995224 Spectral Bands: 0.4 - 2.5 mm

    Pixel: 20m x 20m Scene: 10km x 10km

  • Relevant Material in Applications of Meteorological Satellites

    CHAPTER 2 - NATURE OF RADIATION 2.1 Remote Sensing of Radiation2-12.2 Basic Units2-12.3 Definitions of Radiation 2-22.5Related Derivations2-5

    CHAPTER 3 - ABSORPTION, EMISSION, REFLECTION, AND SCATTERING 3.1Absorption and Emission3-13.2Conservation of Energy3-13.3Planetary Albedo3-23.4Selective Absorption and Emission3-23.7Summary of Interac