Published by Patrick Mutisya · 8 days ago
This note outlines the main stages in the evolution of a typical star, from its birth in an interstellar cloud to its ultimate fate. The description follows the points (a)–(h) required for the Cambridge IGCSE Physics syllabus.
Stars begin in giant clouds of gas and dust, called nebulae. These clouds are primarily composed of hydrogen (\$\sim 90\%\$ by number) with smaller amounts of helium and heavier elements.
Gravitational attraction causes a region of the cloud to collapse. As the material contracts, potential energy is converted into thermal energy, raising the temperature of the core.
When the core temperature becomes high enough (\$\approx 10^7\ \text{K}\$) nuclear fusion of hydrogen into helium starts. The outward pressure from the hot gas balances the inward pull of gravity, establishing hydrostatic equilibrium.
Fusion consumes hydrogen in the core. Eventually the core runs out of hydrogen fuel, and the balance of forces is disturbed.
With hydrogen depleted, the core contracts and heats further, while the outer layers expand and cool, giving the star a reddish appearance.
The red giant sheds its outer layers, creating a glowing planetary nebula. The remaining core, no longer undergoing fusion, becomes a dense white dwarf.
When the core of a red supergiant reaches iron, fusion can no longer release energy. The core collapses catastrophically, producing a supernova. The explosion ejects a nebula enriched with heavy elements. The remnant core becomes:
The supernova nebula, rich in heavy elements, can cool and fragment, forming new interstellar clouds that may eventually collapse to form new stars and planetary systems.
| Stage | Typical Mass Range | Key Processes | Final Remnant |
|---|---|---|---|
| Protostar | 0.1 – 100 \$M_{\odot}\$ | Gravitational collapse, heating | — (becomes main‑sequence star) |
| Main‑sequence star | 0.1 – 100 \$M_{\odot}\$ | Hydrogen fusion (\$4p \rightarrow \,^{4}\!He + 2\gamma + 26.7\ \text{MeV}\$) | — (evolves to giant phase) |
| Red giant (low‑mass) | 0.1 – 8 \$M_{\odot}\$ | Helium fusion, outer envelope expansion | Planetary nebula + white dwarf |
| Red supergiant (high‑mass) | 8 – 30 \$M_{\odot}\$ | Fusion of heavier elements up to iron | Supernova → neutron star |
| Very massive star | \$>30\,M_{\odot}\$ | Rapid fusion, strong stellar winds | Supernova → black hole |
Energy released in hydrogen fusion (main‑sequence phase):
\$4\,^{1}\!H \;\rightarrow\; ^{4}\!He \;+\; 2\,\gamma \;+\; 26.7\ \text{MeV}\$
Hydrostatic equilibrium condition (balance of forces):
\$\frac{dP}{dr} = -\frac{G M(r) \rho(r)}{r^{2}}\$
Schwarzschild radius (relevant for black‑hole formation):
\$R_{s} = \frac{2 G M}{c^{2}}\$