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Large parallax
Star is closer to Earth
Small parallax
Star is farther from Earth
1 arcsecond parallax
Equals 1 parsec of distance
Milli-arcsecond conversion
1000 mas = 1 arcsec
Luminosity definition
Total energy a star emits per second
Apparent brightness
How bright a star appears from Earth; depends on distance
Absolute magnitude
Brightness a star would have at 10 pc
Magnitude scale change
5 magnitudes = 100× brightness change
Magnitude 1 difference
Brightness ratio of 2.512
Smaller B-V color index
Hotter star
Larger B-V color index
Cooler star
Spectral class order
O B A F G K M (hot → cool)
Spectral class numbers
0 = hottest, 9 = coolest
Main-sequence trends
Hotter stars are more massive, luminous, larger, shorter-lived
HR Diagram x-axis
Temperature or spectral class (hot left, cool right)
HR Diagram y-axis
Luminosity or absolute magnitude
Main sequence location
Diagonal band of hydrogen-fusing stars
White dwarf region
Hot but dim (lower-left of HR diagram)
Red giant region
Cool but bright (upper-right of HR diagram)
Luminosity-radius-temperature
L = R²T⁴
Radius doubles
Luminosity increases by factor of 4
Temperature doubles
Luminosity increases by factor of 16
Luminosity classes
I = supergiant, III = giant, V = main sequence
Broad spectral lines
Indicate high gravity (e.g., white dwarfs)
Narrow spectral lines
Indicate low gravity (e.g., supergiants)
Spectroscopic parallax
Spectrum → spectral type → luminosity class → distance
Stellar mass measurement
Only measured accurately using binary stars and Kepler's law
Main-sequence lifetime
Lifetime ∝ 1/mass²·⁵
High mass star lifetime
Shorter main-sequence life
Low mass star lifetime
Longer main-sequence life
Cepheid variables
Period gives luminosity; used as standard candles
Henrietta Leavitt
Discovered Cepheid period-luminosity law
ISM definition
Gas and dust that fills the space between stars
ISM gas composition
Mostly hydrogen: HI, HII, H₂
Gas-to-dust ratio
100 : 1
HI detection
21 cm radio emission
Molecular cloud detection
CO tracer molecules
Extinction
Dust makes stars appear dimmer (magnitude increases)
Reddening
Dust removes blue light more than red light
Emission nebula
HII region glowing from hot O and B stars
Reflection nebula
Blue light from scattering by dust
Dark nebula
Cold molecular gas blocking background light
Molecular clouds
Coldest, densest ISM structures; star formation sites
Hydrostatic equilibrium
Gravity pulling inward = pressure pushing outward
Two stages of star formation
Cloud fragmentation → protostar contraction
Mass vs formation time
High-mass stars form faster
Protostar equilibrium
Not in hydrostatic equilibrium; gravity > pressure
Hayashi track
Evolutionary contraction path of low-mass protostar
Triggered formation
Shockwaves from O/B stars or supernovae trigger star birth
Open cluster
Young, 100s-1000s stars, few parsecs wide
Globular cluster
Old (10-12 Gyr), 10⁵-10⁶ stars in Milky Way halo
Main-sequence turnoff
Hottest star still on MS → determines age
Mass → evolution speed
Higher mass = faster evolution
High-mass star death
Core-collapse (Type II) supernova
Low-mass star death
Planetary nebula → white dwarf
End of main sequence
Core hydrogen exhausted → helium ash core forms
Fusion ash
Material left behind when fusion ends in core
Shell burning
Fusion occurring in layers around core
Helium ignition temperature
~100 million K
Carbon ignition temperature
~600 million K
Triple-alpha process
Helium fusion producing carbon
Main Sequence core
Hydrogen fusion; helium ash buildup
Subgiant Branch core
Helium ash core; hydrogen shell burning
Red Giant Branch core
Inert helium core; strong hydrogen shell burning
Horizontal Branch core
Helium fusion core; hydrogen shell burning continues
AGB core
Carbon-oxygen core; two fusion shells (H + He)
Planetary Nebula core
Hot C/O core ionizing ejected gas
White Dwarf core
Carbon-oxygen degenerate core; no fusion
Fusion limit
Stars cannot fuse elements heavier than iron
Photodisintegration
Gamma rays break iron into helium nuclei during collapse
Neutronization
Electrons + protons → neutrons + neutrinos
Core-collapse rebound
Shockwave produces Type II supernova
Type II supernova
Death of high-mass star; hydrogen present in spectrum
Type Ia supernova
Exploding white dwarf; no hydrogen in spectrum
Chandrasekhar limit
1.4 M☉ maximum white dwarf mass
Type Ia remnant
No remnant left (white dwarf destroyed)
Type Ia brightness
All Type Ia supernovae have same absolute magnitude (M = -19.3)
Big Bang nucleosynthesis
Forms hydrogen, helium, small lithium
Stellar nucleosynthesis
Low mass stars → carbon; high mass stars → iron
s-process
Slow neutron capture in AGB stars
r-process
Rapid neutron capture in supernovae or neutron star mergers
Neutron star formation
Remnant core of Type II supernova
Neutron star size
Radius ~10 km
Neutron degeneracy pressure
Supports neutron stars against gravity
Pulsar
Rotating neutron star with lighthouse-like beams
Black hole formation
Collapse of >3 M☉ core when neutron degeneracy fails
Schwarzschild radius
Distance where escape speed = speed of light
Event horizon
Boundary beyond which nothing escapes
Relativity postulate 1
No absolute reference frame
Relativity postulate 2
Speed of light is constant for all observers
Time dilation
Moving clocks run slower
Gravitational time dilation
Clocks run slower near massive objects
Equivalence principle
Acceleration and gravity are indistinguishable
Gravitational lensing
Light bends around massive objects
Evidence for relativity
Starlight bending, GPS corrections, muon survival, gravitational waves
Spacetime concept
Mass and energy curve spacetime; objects follow curvature