Spectral classes hotβcool: OBAFGKM β 'Oh Be A Fine Girl/Guy, Kiss Me.' Sun = G2V.
OBAFGKM Spectral Classes
The stellar spectral sequence β temperature, color, and what absorption lines reveal
O: >30,000 K β blue, ionized helium lines (Rigel). B: 10,000β30,000 K β blue-white, helium lines (Spica). A: 7,500β10,000 K β white, strong hydrogen (Vega, Sirius). F: 6,000β7,500 K β yellow-white, calcium (Procyon). G: 5,200β6,000 K β yellow, calcium + metals (Sun = G2V). K: 3,700β5,200 K β orange, molecular bands (Arcturus). M: 2,400β3,700 K β red, TiO bands (Betelgeuse). 'V' = main sequence (luminosity class). Extended: L, T, Y for brown dwarfs. Each class has 0β9 subdivisions.
O
Blue, >30,000 K β ionized He
B
Blue-white, 10β30k K β He lines
A
White, 7.5β10k K β H lines
F
Yellow-white, 6β7.5k K
G
Yellow, 5.2β6k K β Sun
K
Orange, 3.7β5.2k K
M
Red, <3,700 K β TiO molecules
Hertzsprung-Russell Diagram
HR diagram: luminosity (y-axis) vs temperature (x-axis, hot LEFT). Main sequence diagonal. Giants upper right. White dwarfs lower left.
Hertzsprung-Russell Diagram
The most important diagram in stellar astronomy β reveals stellar life stages
X-axis: surface temperature (decreasing left to right β hot on left). Y-axis: luminosity (increasing upward). Main sequence: 90% of stars β hydrogen-burning diagonal from hot-luminous (O) to cool-dim (M). Giants/Supergiants: upper right β large, cool, evolved. White dwarfs: lower left β small, hot, evolved. The HR diagram is not a timeline β stars don't move along it continuously. It shows where stars spend most of their time. Mass determines position on main sequence: more massive = hotter, brighter, shorter-lived.
Main sequence
H-burning diagonal β 90% of stars
Giants
Upper right β evolved, large, cool
Supergiants
Top of diagram β most luminous
White dwarfs
Lower left β hot, tiny, dead
Our Sun
G2V β middle of main sequence
Low-Mass Stellar Evolution
Low-mass stars (< ~8 Mβ): main sequence β red giant β planetary nebula β white dwarf β black dwarf.
Low-Mass Stellar Evolution
The life cycle of stars like our Sun β from birth to slow cooling death
Main sequence: H β He fusion in core (~10 billion years for Sun). H exhausted: core contracts, heats β shell burning β star expands β red giant. Helium flash: sudden He ignition in degenerate core. He burning: carbon and oxygen formed. Asymptotic giant branch: double-shell burning, thermal pulses, heavy mass loss. Planetary nebula: outer envelope expelled. White dwarf: remaining carbon-oxygen core, Earth-sized, ~100,000 K β cools over billions of years. Black dwarf: theoretical final state (cooled white dwarf) β none exist yet (universe too young).
High-Mass Stellar Evolution
High-mass stars (> ~8 Mβ): supernova β neutron star or black hole (> ~25 Mβ). Nuclear burning through iron.
High-Mass Stellar Evolution
How massive stars live fast, die violently, and seed the universe with heavy elements
Massive stars: much shorter lives (O stars ~3 million years). Burn through H, He, C, Ne, O, Si in concentric shells (onion structure). Iron: no energy from fusion β iron core grows. Core collapse: when Fe core > 1.4 Mβ (Chandrasekhar limit) β collapse in 0.1 seconds. Type II supernova: bounce creates shock wave β outer layers expelled. Nucleosynthesis: all elements heavier than iron made in supernova. Remnant: neutron star (< ~25 Mβ) or black hole. Supernovae enriched the galaxy with heavy elements β we are made of stardust.
Chandrasekhar Limit
Chandrasekhar limit: 1.4 Mβ β above this, white dwarfs collapse. Basis for Type Ia supernovae as standard candles.
Chandrasekhar Limit
The mass limit for white dwarfs β and why it makes Type Ia supernovae standard candles
Subrahmanyan Chandrasekhar (1930, Nobel 1983): electron degeneracy pressure supports white dwarfs up to 1.4 solar masses. Above this: collapse inevitable. Type Ia supernova: white dwarf in binary accretes mass beyond limit β thermonuclear explosion β same peak luminosity everywhere (standard candle). Used to discover dark energy (1998). Neutron stars: supported by neutron degeneracy pressure up to ~2β3 Mβ (Tolman-Oppenheimer-Volkoff limit). Above TOV limit: black hole inevitable.
Nuclear Fusion in Stars
Stellar fusion: pp-chain (Sun), CNO cycle (massive stars). Energy = mass deficit Γ cΒ². 4H β He-4 + energy.
Stellar Nucleosynthesis
How stars convert hydrogen to helium β and eventually forge all elements up to iron
Proton-proton (pp) chain: dominates in stars < 1.5 Mβ. 4 protons β He-4 + 2 positrons + 2 neutrinos + energy. Mass deficit: He-4 is 0.7% lighter than 4 protons β E = mcΒ². Sun converts 4 million tons/sec to energy. CNO cycle: dominates in massive stars β carbon/nitrogen/oxygen act as catalysts. Helium burning: 3 He-4 β C-12 (triple-alpha). Carbon burning: C β Ne, Mg. Each stage produces heavier elements up to iron. Iron: most stable nucleus β fusion would require energy input. End of the line.
Neutron Stars
Neutron stars: ~1.4 Mβ in ~20 km diameter. Density: 1 teaspoon = billion tons. Spin up to 700 Hz (millisecond pulsars).
Neutron Stars
The densest visible objects in the universe β a city-sized remnant of a supernova
Formed in core-collapse supernovae. Mass: ~1.4 Mβ. Radius: ~10 km. Density: neutrons packed at nuclear density β 1 tsp β 10βΉ kg. Strong magnetic fields: up to 10ΒΉβ΅ Gauss (magnetars). Pulsars: rotating neutron stars with radio beams sweeping like a lighthouse β extremely regular β used as cosmic clocks. Millisecond pulsars: spun up by accretion in binary β hundreds of rotations/second. GW170817: neutron star merger detected in gravitational waves + light β kilonova β heavy elements (gold, platinum) created.
Black Holes
Black holes: gravity so strong even light can't escape. Event horizon: point of no return. Schwarzschild radius = 2GM/cΒ².
Black Holes
The most extreme objects in physics β predicted by Einstein, confirmed by observation
Event horizon: boundary from which nothing escapes, r_s = 2GM/cΒ². Stellar black holes: from > ~25 Mβ stellar collapse. Intermediate: 100β10β΅ Mβ (evidence accumulating). Supermassive: 10βΆβ10ΒΉβ° Mβ in galactic centers. First image: M87* (2019, Event Horizon Telescope), Sgr A* (2022). Hawking radiation: quantum effect β black holes slowly evaporate (not yet observed). Tidal forces (spaghettification) at stellar black holes. No 'singularity' in quantum gravity theories. Information paradox: still unresolved.
Variable Stars
Variable stars: change brightness. Cepheids (pulsation) β standard candles. Novae: binary mass transfer explosions.
Variable Stars
Stars whose brightness changes β and how they revolutionized distance measurement
Intrinsic variables: Cepheids (pulsation period 1β100 days, period β luminosity β Henrietta Leavitt 1908), RR Lyrae, Mira (red giant pulsation). Eruptive: T Tauri (young), flare stars. Extrinsic: eclipsing binaries (Algol), rotating spotted stars. Leavitt's period-luminosity law: revolutionized distance measurement β Cepheids are standard candles to ~100 Mpc. Hubble used Cepheids in Andromeda to prove it was a separate galaxy (1924). Type Ia supernovae: even brighter standard candles β dark energy discovery.
Star Formation
Stars form in molecular clouds. Jeans instability: cloud collapses when gravity > pressure. Protostar β T Tauri β main sequence.
Star Formation
How molecular clouds collapse into newborn stars β from gas to nuclear fusion
Molecular clouds: cold (10β30 K), dense, mostly Hβ and CO. Jeans instability: if cloud mass > Jeans mass, gravity wins over thermal pressure β collapse. Collapse: conservation of angular momentum β rotation β protoplanetary disk. Protostar: heating by gravitational contraction (not yet fusion). T Tauri stage: nuclear reactions begin, strong stellar winds clear surrounding nebula. Main sequence: hydrogen fusion begins β hydrostatic equilibrium. Time to main sequence: ~50 million years for Sun-like star. HII regions: ionized gas glowing around hot young stars (Orion Nebula).
Binary Stars
~50% of Sun-like stars in binary systems. Mass transfer can create novae, X-ray binaries, and Type Ia supernovae.
Binary Star Systems
More than half of all stars have companions β with dramatic consequences
Visual binaries: both stars resolved (Albireo). Spectroscopic binaries: Doppler shifts reveal orbital motion. Eclipsing binaries: brightness dips as stars transit each other β gives radii and masses. Mass transfer: evolved giant fills Roche lobe β mass flows to companion. Cataclysmic variables: white dwarf + main sequence β accretion, nova explosions. X-ray binaries: neutron star or black hole + companion β accretion disk β X-ray emission. Type Ia supernova: white dwarf accretes β exceeds Chandrasekhar limit β thermonuclear explosion. Gravitational wave source: compact binary mergers.
Stellar Distances
Distances: parallax (nearby), Cepheids (intermediate), Type Ia SN (distant). 1 parsec = 3.26 light-years.
Measuring Stellar Distances
The cosmic distance ladder β the foundation of all extragalactic astronomy
Parsec: distance at which 1 AU subtends 1 arcsecond. 1 pc = 3.26 ly. Nearest star: Proxima Centauri, 1.3 pc = 4.24 ly. Parallax: trigonometric, accurate to ~10 kpc with Gaia. Proper motion: star's real movement across sky. Spectroscopic parallax: spectral type β luminosity β distance (less accurate). Standard candles: Cepheids, RR Lyrae, Type Ia SN. Light-year vs parsec: astronomers use parsecs; popular science uses light-years. Megaparsec (Mpc) = 3.26 million light-years used for extragalactic distances.