Fig. 5

Eclipse magnitude ϒ, defined in Eq. (14), vs. displacement l of the shadow trace, for radii s1 = 2s2 (left) and s1 = 3s2 (right). The visuals show the viewpoint from the star: the eclipses (both types) trace out a nearly horizontal band. Blue and red: ϒ and
for lunar andplanetary eclipses, respectively. For |l| = s1 ± s2, the shadow cylinder of one partner grazes its companion (and the projected disks touch). There, the third derivative is infinite, resulting in a tail in the Fourier spectrum. When ϒ(lk) is multiplied with the phase curve h(ϑk − ϕo), one obtains |g(ϑk)| which equals the integrated dip in the light curve for edge-on observation of an eclipse.
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