4.2 White Dwarf Physics and Chandrasekhar Limit
Updated August 2024Fiveable Content Team
🚀Astrophysics II Unit 4 Review
4.2 White Dwarf Physics and Chandrasekhar Limit
🚀 Astrophysics II
Unit 4 – Supernovae and Compact Stellar Remnants
White dwarfs are fascinating stellar remnants that mark the end of most stars' lives. These dense objects, supported by electron degeneracy pressure, have an inverse mass-radius relationship and come in various compositions.
The Chandrasekhar limit, a crucial concept in white dwarf physics, sets the maximum mass for these stars at about 1.44 solar masses. This limit plays a key role in understanding stellar evolution, supernovae, and cosmic distance measurements.
White Dwarf Structure
Electron Degeneracy Pressure and Mass-Radius Relationship
- Electron degeneracy pressure supports white dwarfs against gravitational collapse
- Quantum mechanical effect prevents electrons from occupying same energy states
- Results in an inverse mass-radius relationship for white dwarfs
- More massive white dwarfs have smaller radii due to increased gravitational compression
- Typical white dwarf mass ranges from 0.6 to 1.4 solar masses
- Radii of white dwarfs generally fall between 0.008 and 0.02 solar radii (comparable to Earth's size)
Composition and Types of White Dwarfs
- Carbon-oxygen white dwarfs comprise the majority of observed white dwarfs
- Form from low to intermediate-mass stars (up to about 8 solar masses)
- Carbon and oxygen produced through helium fusion in the star's core
- Helium white dwarfs exist but are less common
- Result from binary star evolution or very low-mass stars
- Consist primarily of helium with a thin hydrogen envelope
- Oxygen-neon-magnesium white dwarfs form from more massive progenitor stars
- Rare type of white dwarf with masses approaching the Chandrasekhar limit

White Dwarf Evolution
Cooling Sequence and Spectral Changes
- White dwarfs gradually cool over billions of years
- Initial surface temperatures can exceed 100,000 K
- Cooling follows a predictable sequence used to estimate white dwarf ages
- Spectral classification changes as the white dwarf cools
- Hot white dwarfs show strong helium lines (DB spectral type)
- Cooler white dwarfs display prominent hydrogen lines (DA spectral type)
- Cooling rate slows significantly at lower temperatures due to decreased thermal energy loss
- Oldest white dwarfs in our galaxy have cooled to temperatures around 4,000 K

Accretion Processes and Binary Systems
- White dwarfs in binary systems can accrete matter from companion stars
- Accretion increases the white dwarf's mass and can lead to various phenomena
- Classical novae occur when accreted hydrogen undergoes thermonuclear fusion
- Type Ia supernovae result from white dwarfs approaching the Chandrasekhar limit
- Accretion disks form around white dwarfs in close binary systems
- Disks emit X-rays and ultraviolet radiation due to high temperatures
- Magnetic white dwarfs can channel accreted material along magnetic field lines
- Creates hot spots on the white dwarf's surface (AM Herculis stars)
White Dwarf Limits
The Chandrasekhar Limit and Its Implications
- Chandrasekhar limit defines the maximum mass of a stable white dwarf
- Theoretical upper limit calculated to be approximately 1.44 solar masses
- Derived from the balance between electron degeneracy pressure and gravity
- White dwarfs approaching this limit become unstable
- Electron capture by protons reduces electron degeneracy pressure
- Can lead to collapse into a neutron star or trigger a Type Ia supernova
- Chandrasekhar limit plays a crucial role in understanding stellar evolution and supernovae
- Provides a standard candle for measuring cosmic distances (Type Ia supernovae)
- Recent observations suggest some white dwarfs may slightly exceed the limit
- Rotation or strong magnetic fields might provide additional support