Planetary Nebulae 1983
DOI: 10.1007/978-94-009-7094-6_22
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On the O III/O II Problem in Medium and High Excitation Planetary Nebulae

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“…When the He  λ4686 line was too weak to be measured, we determined its upper limit so as to derive an upper limit to the temperature of the central star. These cases correspond to T marked with b in Table 1 Che & Köppen 1983) In the other cases, models with different nebular radii were built. For these PNe we found the smallest and the largest radius for which the model converged.…”
Section: The Modelling Proceduresmentioning
confidence: 99%
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“…When the He  λ4686 line was too weak to be measured, we determined its upper limit so as to derive an upper limit to the temperature of the central star. These cases correspond to T marked with b in Table 1 Che & Köppen 1983) In the other cases, models with different nebular radii were built. For these PNe we found the smallest and the largest radius for which the model converged.…”
Section: The Modelling Proceduresmentioning
confidence: 99%
“…The optical depth of the nebula is derived from the hydrogen ionization structure predicted by the is not only sensitive to the size of the nebula, but it also depends also on several other parameters, mainly on the density distribution (cf. Che & Köppen 1983). When T is derived from the upper limit of the He  λ4686 line, only an upper limit to the helium and other metal abundances can be derived.…”
Section: The Modelling Proceduresmentioning
confidence: 99%