Fig. 1.

Angular dependence of the radiative force parameter for models M1, M2, and M3 (when M(τ) = 0; thin dashed lines) and models ,
, and
(when M(τ)≠0; thick lines). The horizontal line marks the value
. Just below this value, the matter undergoes a pure accretion process (type 1 solution), while above this value, it transitions to a type 5 outflow solution (which we discard). Each pair of models (Mi,
) uses the same boundary conditions.
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