Degenerate electrons conduct heat efficiently, making most of the interior nearly isothermal while an outer nondegenerate insulating envelope sustains a large temperature gradient. Nuclei have much larger masses and much smaller thermal de Broglie wavelengths than electrons, so their quantum degeneracy is weak at these temperatures/densities, although Coulomb coupling and crystallization can matter. Under the stipulated classical ideal-carbon-ion approximation,This excludes crystallization, latent heat and low-temperature heat-capacity changes; nondegenerate does not automatically mean weakly interacting.
U=2312muMkBTc=8muMkBTc.
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