Fig. 3

The sketch demonstrates how a differential element of solid angle dΩ fans out when traced sunwards from the observer’s site. The dashed line represents the trajectory passing through the middle-point of the solid angle element. In a transparent atmosphere, the ratio of radiance and the squared refraction index is conserved on the ray trajectory, and the corresponding irradiance for the differential solid angle element is simply L(xO,sO)sO·nxOdΩ(sO) ~ L(x⊙,s⊙)dΩ(sO). For the calculation of Eq. (3), a mathematical transformation is applied to rewrite the integral in the auxiliary variables ξ and η.
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