1976
DOI: 10.1175/1520-0469(1976)033<2452:tdeafr>2.0.co;2
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The Delta-Eddington Approximation for Radiative Flux Transfer

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Cited by 1,004 publications
(538 citation statements)
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“…The delta-Lddington approximation of the radiative transfer equation (Joseph et al 1976), which is designed for strongly asymmetric scattering medium, gives the scattering transmission coefficient as _r*64…”
Section: Parameterization Fc)uationsmentioning
confidence: 99%
“…The delta-Lddington approximation of the radiative transfer equation (Joseph et al 1976), which is designed for strongly asymmetric scattering medium, gives the scattering transmission coefficient as _r*64…”
Section: Parameterization Fc)uationsmentioning
confidence: 99%
“…This approximation is valid for a medium that shows strong forward scattering [13]. For large particle diameter-to-wavelength ratios of over I00 (as is the case here), asymptotic approximations yield accurate results with minimal computational complexity [14].…”
Section: A Near-infrared Reflectancementioning
confidence: 99%
“…The directional hemispherical reflectance, R, is then calculated at a specific angle of incidence, θ, from [13] …”
Section: A Near-infrared Reflectancementioning
confidence: 99%
“…(6.14)]; furthermore, as the only intensity I * (T, *) determines the fluxes, the relevant equation [Liou, 1980, Eq. (6.22)] constitutes the azimuthally averaged form of RTE and is the starting point for a variety of approximate methods, which by use of simple expressions for P(cos *) mainly determine radiative fluxes (Wiscombe and Joseph, 1977;Joseph et al, 1976;Liou, 1974;Schaller, 1979;Meador and Weaver, 1980). The moments xn always enter the various expressions assumed by the phase function within these forms of RTE.…”
Section: Computationsmentioning
confidence: 99%
“…The Eddington and the Two-Stream methods have been improved by the Delta-Eddington (Joseph et al, 1976) and the Delta-Two-Stream (Schaller, 1979) methods by making use of the *-approximation to the phase function, which combines a delta function expressing the contribution of the forward peak with two terms depending on *. An extension of the *-approximation is the *-M approximation (Wiscombe, 1977), which expresses the phase function as a delta function plus 2M terms depending on * (for M=1 one gets the above *-approximation) ; an example of using this approximation in connection with the spherical harmonics method, leading to the the Delta-Spherical Harmonics method, can be found in Kondratyev et al (1981).…”
Section: Computationsmentioning
confidence: 99%