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Fig. 16

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Effective temperatures of embedded cores as a function of the central pressure in the filament, which is assumed to be either a self-gravitating sphere or a self-gravitating cylinder. In case a), the dust emissivities are the apparent values of the modified back-body appromixation, while in b) the apparent emissivities are increased by a factor 8. The external pressure outside of the filaments is assumed to be 2  ×  104, 105, and 106   K/cm3. The filaments are heated either by the ISRF as provided by Mathis et al. (1982) (grey lines) or by an ISRF where the diffuse dust emission is added.

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