A helium flash is a very brief thermal runaway nuclear fusion of large quantities of helium into carbon through the triple-alpha process in the core of low mass stars (between 0.8 solar masses (M☉) and 2.0 M☉) during their red giant phase (the Sun is predicted to experience a flash 1.2 billion years after it leaves the main sequence). A much rarer runaway helium fusion process can also on the surface of accreting white dwarf stars. Due to the inability of these low mass stars to counter the pressure of gravity by fusing helium when the hydrogen in the core is exhausted, eventually a flash of very intense helium fusion (or burning) occurs because the accumulation of helium which has become degenerate matter has reached a certain percentage of the total helium in the core where it is supported against gravitational collapse by quantum mechanical pressure rather than thermal pressure. This process causes an increase in the temperature and density of the core which then finally does undergo helium burning when the core reaches 100 million kelvins but at a tremendous rate because this burning does not act to expand the matter against the pressure of gravity and hence cool it (as does happen in main sequence stars which burn too much hydrogen) because it is degenerate, and a fundamental quality of degenerate matter is that changes in temperature will not affect the volume of the mass, and thus there is no regulation of the rate of fusion through hydrostatic equilibrium. The very high density speeds up the fusion rate until there is a runaway nuclear reaction which lasts a few minutes and which briefly emits energy at a rate comparable to the whole Milky Way. In the case of normal low mass stars, the energy is absorbed by the star and thus is undetected by observation and is solely described by astrophysical models. The process ends when the material is heated to the point where thermal pressure again becomes dominant, and the material then expands and cools. It is estimated that the electron-degenerate helium core weighs about 40% of the star mass and that 6% of the core is converted into carbon.
During the red giant phase of stellar evolution in stars with less than 2.0 M☉ the nuclear fusion of hydrogen ceases in the core as it is depleted, leaving a helium-rich core. While fusion of hydrogen continues in the star’s shell causing a continuation of the accumulation of helium ash in the core, making the core denser, the temperature still is unable to reach the level required for helium fusion, as happens in more massive stars. Thus the thermal pressure from fusion is no longer sufficient to counter the gravitational collapse and create the hydrostatic equilibrium found in most stars. This causes the star to start contracting and increasing in temperature until it eventually becomes compressed enough for the helium core to become degenerate matter. This degeneracy pressure is finally sufficient to stop further collapse of the most central material but the rest of the core continues to contract and the temperature continues to rise until it reaches a point (×108 K) at which the helium can ignite and start to fuse. ≈1
The explosive nature of the helium flash arises from its taking place in degenerate matter. Once the temperature reaches 100 million–200 million kelvins and helium fusion begins using the triple-alpha process, the temperature rapidly increases, further raising the helium fusion rate and, because degenerate matter is a good conductor of heat, widening the reaction region.
However, since degeneracy pressure (which is purely a function of density) is dominating thermal pressure (proportional to the product of density and temperature), the total pressure is only weakly dependent on temperature. Thus, the dramatic increase in temperature only causes a slight increase in pressure, so there is no stabilizing cooling expansion of the core.
This runaway reaction quickly climbs to about 100 billion times the star's normal energy production (for a few seconds) until the temperature increases to the point that thermal pressure again becomes dominant, eliminating the degeneracy. The core can then expand and cool down and a stable burning of helium will continue.
A star with mass greater than about 2.25 M☉ starts to burn helium without its core becoming degenerate, and so does not exhibit this type of helium flash. In a very low-mass star (less than about 0.5 M☉), the core is never hot enough to ignite helium. The degenerate helium core will keep on contracting, and finally becomes a helium white dwarf.
The helium flash is not directly observable on the surface by electromagnetic radiation. The flash occurs in the core deep inside the star, and the net effect will be that all released energy is absorbed by the entire core, leaving the degenerate state to become nondegenerate. Earlier computations indicated that a nondisruptive mass loss would be possible in some cases, but later star modeling taking neutrino energy loss into account indicates no such mass loss.
Binary white dwarfs
When hydrogen gas is accreted onto a white dwarf from a binary companion star, the hydrogen can fuse to form helium for a narrow range of accretion rates, but most systems develop a layer of hydrogen over the degenerate white dwarf interior. This hydrogen can build up to form a shell near the surface of the star. When the mass of hydrogen becomes sufficiently large, runaway fusion causes a nova. In a few binary systems where the hydrogen fuses on the surface, the mass of helium built up can burn in an unstable helium flash. In certain binary systems the companion star may have lost most of its hydrogen and donate helium-rich material to the compact star. Note that similar flashes occur on neutron stars.
Shell helium flash
Shell helium flashes are a somewhat analogous but much less violent, nonrunaway helium ignition event, taking place in the absence of degenerate matter. They occur periodically in asymptotic giant branch stars in a shell outside the core. This is late in the life of a star in its giant phase. The star has burnt most of the helium available in the core, which is now composed of carbon and oxygen. Helium fusion continues in a thin shell around this core, but then turns off as helium becomes depleted. This allows hydrogen fusion to start in a layer above the helium layer. After enough additional helium accumulates, helium fusion is reignited, leading to a thermal pulse which eventually causes the star to expand and brighten temporarily (the pulse in luminosity is delayed because it takes a number of years for the energy from restarted helium fusion to reach the surface). Such pulses may last a few hundred years, and are thought to occur periodically every 10,000 to 100,000 years. After the flash, helium fusion continues at an exponentially decaying rate for about 40% of the cycle as the helium shell is consumed. Thermal pulses may cause a star to shed circumstellar shells of gas and dust.
- Chapter 9: Post-main sequence evolution through helium burning
- The End Of The Sun
- "White Dwarf Resurrection". Retrieved 3 August 2015.
- Hansen, Carl J.; Kawaler, Steven D.; Trimble, Virginia (2004). Stellar Interiors - Physical Principles, Structure, and Evolution (2 ed.). Springer. pp. 62–5. ISBN 978-0387200897.
- Seeds, Michael A.; Backman, Dana E. (2012). Foundations of Astronomy (12 ed.). Cengage Learning. pp. 249–51. ISBN 978-1133103769.
- Karttunen, Hannu; Kröger, Pekka; Oja, Heikki; Poutanen, Markku; Donner, Karl Johan (eds.). Fundamental Astronomy (5 ed.). Springer. p. 249. ISBN 978-3540341437.
- Deupree, R. G.; R. K. Wallace (1987). "The core helium flash and surface abundance anomalies". Astrophysical Journal 317: 724–732. Bibcode:1987ApJ...317..724D. doi:10.1086/165319.
- Two- and three-dimensional numerical simulations of the core helium flash by Deupree, R. G.
- A Reexamination of the Core Helium Flash by Deupree, R. G.
- Multidimensional hydrodynamic simulations of the core helium flash in low-mass stars by Mocák, M.
- Wood, P. R.; D. M. Zarro (1981). "Helium-shell flashing in low-mass stars and period changes in mira variables". Astrophysical Journal 247 (Part 1): 247. Bibcode:1981ApJ...247..247W. doi:10.1086/159032.