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Phase function is the scattering function normalized by the scattering coefficient, b. For axially-symmetrical scattering functions, i.e. scattering functions that depend only on the scattering angle, the phase function, usually denoted by p [steradian-1], is defined as follows:
| p(θ) = β(θ) / b | (1) |
The phase function can be regarded as a distribution of probability of a photon being scattered at an angle θ. Indeed, for an axially-symmetrical phase function we have:
| 2π ∫0π p(θ) sinθ dθ | = [ 2π ∫0π β(θ) sinθ dθ ] / b | |
| = b / b | ||
| = 1 | (2) |
i.e. a normalization condition required of a probability distribution. The factor of 2π in the above equation arises from an integration over the azimuth angle over its full range: from 0 to 2π.
Note that another definition of the phase function is popular in the radiative transfer literature (for example, Kokhanovsky 2004, Liou and Hansen 1971):
| p(θ) = 4π β(θ) / b | (3) |
leading to a normalization condition different from that expressed by Eq. 2 (for example, Kokhanovsky 2004, Haltrin 1998):
| ½ ∫0π p(θ) sinθ dθ = 1 | (4) |
See also: Scattering matrix for a dispersion .. .
| CITATION: Jonasz M. 2006. Phase function (www.tpdsci.com/Tpc/ScaPhsFn.php). In: Top. Part. Disp. Sci. (www.tpdsci.com). |
HISTORY: Published: 17-Jan-2006 Modified: 20-Jul-2006 Peer-reviewed: 11-Oct-2006 |
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