A Second Kelvin-Helmholtz Timescale of Post Helium-Flash Evolution
Andrew Gould

TL;DR
This paper reveals a second Kelvin-Helmholtz timescale governing the post-helium-flash evolution of stars, driven by core contraction, which influences the star's return to stable nuclear fusion.
Contribution
It identifies and characterizes a second Kelvin-Helmholtz timescale in post-helium-flash stellar evolution, highlighting the role of gravitational contraction in star luminosity regulation.
Findings
The first Kelvin-Helmholtz timescale is about 10,000 years.
The second Kelvin-Helmholtz timescale is about 1 million years.
Core contraction governs the star's return to nuclear fusion.
Abstract
I show that after the "helium flash" abruptly ends its first ascent red giant evolution, a solar-type star is powered primarily by gravitational contraction of its helium core, rather than by nuclear fusion. Because this energy is released in the core rather than the envelope, the overall structure of the star, and so its luminosity, is driven toward that of a red clump star from its initial position at the tip of the red giant branch (TRGB). This occurs on a first (and well recognized) Kelvin-Helmholtz timescale t_{KH,1} ~ E_env/L_TRGB ~ 1e4 yrs., where E_env is the thermal energy stored in the envelope and L_TRGB is the luminosity at the TRGB. However, once the star assumes the approximate structure of a clump star, it remains powered primarily by contraction for a {\it second} Kelvin-Helmholtz timescale t_{KH,2} ~ E_core/L_clump ~ 1e6 yrs, where E_core is the thermal energy stored in…
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Taxonomy
TopicsStellar, planetary, and galactic studies · Quantum, superfluid, helium dynamics · Quantum chaos and dynamical systems
