Fig. 4.

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Variation with frequency of the normalized source function at τ ≈ 1, for different values of the velocity-changing elastic collision parameter ζ (indicated in the top-left frame). The model-atmosphere is the same as the one considered in Sect. 6 and Hummer (1969). As expected, successive solutions range between standard PRD-RI − A values (blue) and the limit of the CRD solution (dashed line) for increasing values of ζ.
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