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Chapter 3 Radiative transfer processes in the aquatic medium Remote Sensing of Ocean Color Instructor: Dr. Cheng-Chien LiuCheng-Chien Liu Department of Earth Science National Cheng-Kung University Last updated: 13 March 2003
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3.1 Incident light Incident sky irradiance Rigorous models of surface irradiance HITRAN, FASCODE, LOWTRAN, … the size and computational complexity of these models impractical for many oceanographic applications Simple atmospheric radiative transfer models (Justus and Paris, 1985) (Bird and Riordan, 1986) (Green and Chai, 1988) Pros: Simple Both direct and diffuse irradiance are calculated globally Cons: Specific to continental aerosols
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3.1 Incident light (cont.) Incident sky irradiance (cont.) A simple spectral solar irradiance model for cloudless maritime atmospheres (Gregg and Carder 1990)
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3.1 Incident light (cont.) Cloud effect Kasten and Czeplak (1980)
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3.1 Incident light (cont.) Incident sky radiance Crude approximation A heavily overcast day cardioidal distribution e.g. L( , ) = L 0 (1+2cos ), 0 /2 A cloudless day a collimated direct solar beam plus an isotropic diffuse sky radiance
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3.1 Incident light (cont.) Incident sky radiance (cont.) A cloud cover model of sky radiance Harrison and Coombes (1988).
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3.1 Incident light (cont.) Incident sky radiance (cont.) A cloud cover model of sky radiance (cont.) The normalized sky radiance N( , ) can be given analytically by combining the normalized overcast sky radiance N o ( , ) and the normalized clear sky radiance N c ( , ) where is the sky zenith angle, is the sky azimuth angle relative to the Sun, s is the solar zenith angle, and is the scattering angle between sky and the Sun directions.
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3.2 Transmission across the air-water interface The level surface Refraction – Snell’s law Air-incident case Water-incident case
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Fig. 3.2.1 Fig. 3.2.1 Schematic diagrams for trajectories of photons passing through a flat air- water surface. Redrawn from (Mobley 1994)
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3.2 Transmission across the air-water interface (cont.) Reflection – Fresnel’s equation Air-incident case Water-incident case
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Fig. 3.2.2 Fresnel reflectance function Fig 3.2.2
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3.2 Transmission across the air-water interface (cont.) Capillary waves The relation between the mean-square wave slope 2 over the sea surface and the surface wind speed V wind can be described by an equation proposed by Cox and Munk (1954) 2 = 0.003 + 0.00512V wind
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3.2 Transmission across the air-water interface (cont.) Capillary waves (cont.) The probability function P( ws ) of the occurrence of wave slope where ws is the angle between the vertical and the normal to the sea surface at a given point
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3.2 Transmission across the air-water interface (cont.) Whitecaps effect The probability of reflectance can be further corrected by taking the white cap effect into consideration (Kirk 1994)
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3.3 Radiative transfer process within the aquatic medium Path length The path length of a photon before it hits another particle (Gordon 1994) where j is a sequence of random numbers between 0 and 1 explanation
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3.3 Radiative transfer process within the aquatic medium (cont.) Absorption Bio-optical model of absorption (Prieur and Sathyendranath 1981)
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3.3 Radiative transfer process within the aquatic medium (cont.) Scattering Bio-optical model of scattering (Gordon et al. 1983, Morel 1991)
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3.3 Radiative transfer process within the aquatic medium (cont.) Probability of photon survival
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3.3 Radiative transfer process within the aquatic medium (cont.) Direction of scattering The average VSF derived from Petzold’s measurements (Mobley 1994) Henyey-Greenstein phase function (1941) Fournier-Forand phase function (1994)
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3.4 Bottom boundary Lambertian assumption Bi-directional reflectance Reflectance of various bottom types
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Fig. 3.4.1 Reflectance of various bottom types Fig 3.4.1
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3.5 Radiative transfer equation Classic radiative transfer equation
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Fig. 3.5.1 Illustration of radiative transfer equation
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