MODULE:KNOWLEDGE-BASE
SIMULATION: ACTIVE
RETURN::Stellar Physics

Stellar Nucleosynthesis

How Stars Forge the Elements

Massive Star Interior — Onion Shell

Cross-section of a ~25 M☉ star moments before core collapse. Shells are not to scale — the H envelope normally accounts for >99% of the radius. Each layer fuses progressively heavier elements at higher temperatures.

The Fusion Hierarchy

Each fusion stage requires a higher temperature than the last because heavier nuclei carry larger Coulomb barriers. As the core ash from one stage builds up, gravity compresses and heats it until the next reaction ignites.

Heavier fuels burn dramatically faster — H lasts millions of years, Si just a single day. Once iron forms, fusion can no longer release energy and the core collapses in under a second.

Lower-mass stars stop early. The Sun will fuse only H and He, then shed its envelope as a planetary nebula — leaving a carbon-oxygen white dwarf.

Origins of the Elements
Big Bang nucleosynthesisH, He, traces of Li
Cosmic ray spallationLi, Be, B
Low-mass stars (AGB)C, N, F, s-process up to Pb
Massive stars + Type II SNO, Ne, Mg, Si, S, Ca, Fe-peak
Type Ia supernovaeMost Fe-group isotopes
Neutron star mergers (r-process)Au, Pt, U, lanthanides

Every atom heavier than helium in your ship was forged by stars or stellar explosions.

ED: Material Origins

Common materials — carbon, iron, nickel — are abundant because they sit at energy minima of stellar fusion. The iron peak is where every massive star ends.

Rare materials — technetium, ruthenium, polonium — require explosive r-process synthesis. They are signatures of neutron star mergers and supernova remnants, which is why they cluster around the galaxy's most violent regions.

The Iron Peak hand-in materials and exotic super-heavy elements in jumponium recipes trace back directly to the physics shown here.

Fusion Stages — 25 M☉ Reference
StageFuelProductCore TDurationNote
Hydrogen burningHHe~15 MK~7 MyrProton-proton chain & CNO cycle
Helium burningHeC, O~200 MK~700 kyrTriple-alpha process
Carbon burningCNe, Mg, Na~900 MK~600 yrOnset of neutrino-dominated cooling
Neon burningNeO, Mg~1.7 GK~1 yrPhotodisintegration kicks in
Oxygen burningOSi, S, Ar~2.3 GK~6 moMassive neutrino energy losses
Silicon burningSiFe, Ni~3.5 GK~1 dayLast exothermic stage
Core collapseFe~5 GK<1 secPhotodisintegration → supernova