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46, where a spherical harmonic expansion is introduced for the radiance. In Appendix A, Eq. 25) is introduced using an intuitive physical reasoning. The second simplifying assumption assumes that the time variation of the diffuse flux vector J(r, t) over a time range ∆t = 1/(vµs ) is negligible with respect to the vector itself and can be expressed as7 1 ∂ J(r, t) ∂t vµs J(r, t) . 26) With Eq. 26), “slow” time variations of the flux are therefore assumed. , I(r, sˆ) = 1 3 Φ(r) + J(r) · sˆ. 27) In general, Eqs.

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