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Fig. 4

image

Schematic of the numerical problem. The (independent) grid parameter m ranges from the core mass Mcore to the (unknown) total mass M. The five structure equations for P, T, r, Mz, and E are solved byimposing ten boundary conditions. The radii Rcore and Rout follow from Mcore and M, respectively, and MZ,tot is incremented according to the time-step Δt, ΔMZ,tot = pebΔt. The total energy E is needed to provide the luminosity L at any point (Eq. (10)). In Phase II, Mcore becomes a known parameter, while the metallicity threshold parameter Zmax is added as an unknown.

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