Lecture 16: The Evolution Of Low-Mass Stars

White Dwarf star

Main Sequence Phase

Energy Source: Hydrogen fusion in the core

What happens to the He created by H fusion?

  • Core is too cool to ignite He fusion
  • Slowly builds up an inert He core

Main-Sequence (H-burning) Lifetime:

  • ~10 Gyr for a 1 Msun star (e.g., Sun)
  • ~10 Tyr for a 0.1 Msun star (red dwarf)

Core Hydrogen Exhaustion

Inside:
  • He core collapses & starts to heat up.
  • H burning zone moves into a thin shell surrounding the core
  • Collapsing core heats the H shell above it, driving the fusion faster.
  • More fusion = more heating, so that Pressure > Gravity
Red Giant Star Interior

Outside:

  • Envelope expands and cools
  • Star gets brighter and redder & climbs up the Giant Branch.
Red Giant Branch on H-R Diagram

Climbing the Red Giant Branch

It takes a star about 1 Gyr to climb the Red Giant Branch
  • He core contracting & heating, but no fusion
  • H burning to He in a shell around the core
  • Huge, puffy envelope ~ size of orbit of Venus
At the Tip of the Red Giant Branch:
  • Tcore reaches 100 Million K
  • Ignite He burning in the core in a flash.

Helium Flash

At 100 Million K, a new fusion source ignites: the Triple-alpha Process.

This is the fusion of three 4He nuclei into one 12C (carbon) nucleus through a multi-step nuclear reaction chain that involves the momentary formation of 8Be:

Triple-Alpha Process

Once Carbon is formed, a secondary reaction forms Oxygen from the fusion of Carbon & Helium:

C12-Alpha-Gamma Reaction

When this occurs, the star once again has a nuclear power source in its core and leaves the Giant Branch.

Inside:

  • Starts generating primary energy from He burning in the core.
  • Gets additional energy from an H burning shell surrounding the core.

Outside:

  • Gets hotter and bluer.
  • Star shrinks in radius, getting fainter.

The new energy source helps the star begin to regain Hydrostatic and Thermal Equilibrium. As it does so, it moves onto the Horizontal Branch.

He Flash to Horizontal Branch on the H-R Diagram

Horizontal Branch Phase

Structure:
  • He-burning core
  • H-burning shell
Horizontal Branch Star Interior

The Triple-alpha Process is very inefficient at producing energy, so it can only last for about 100 Myr.

While it goes on, the star steadily builds up a C-O core, but it is still too cool to ignite Carbon fusion

Asymptotic Giant Branch Phase

After 100 Myr, the core runs out of Helium for Triple-Alpha fusion.

Inside:

  • C-O core collapses and heats up
  • He burning shell outside the C-O core
  • H burning shell outside the He burning shell

Asymptotic Giant Branch Star Interior

Outside:

  • Star grows rapidly in radius and cools

Climbs the Giant Branch again, but at a higher effective Temperature than the Giant Branch, so it ascends with a bluer color, putting it slightly to the left of the original Giant Branch on the H-R Diagram: Asymptotic Giant Branch on the H-R diagram

The star becomes an Asymptotic Giant Branch Star

The Instabilities of Old Age

He burning is very temperature sensitive: Triple-alpha fusion rate ~ T40!

Consequences:

  • Small changes in T lead to
  • Large changes in fusion energy output

Star experiences huge Thermal Pulses that destabilize the outer envelope.

Core-Envelope Separation

Rapid Process: takes ~105 years

Outer envelope gets slowly ejected (fast wind)

C-O core continues to contract:

  • With the weight of envelope taken off, the core heats up less
  • It never reaches the Carbon fusion ignition temperature of 600 Million K

Core and Envelope separate physically.

Planetary Nebula Phase

Expanding envelope forms a nebula around the contracting C-O core:
  • Ionized and heated by the hot central core.
  • Expands away to nothing in ~104 years.

The star briefly becomes host to a Planetary Nebula

The hot C-O core is exposed, and moves quickly to the left on the H-R Diagram at nearly constant luminosity and increasing temperature. Final Stages: Envelope Ejection to White Dwarf

Images of Planetary Nebulae

Planetary nebulae are among the most beautiful objects in the sky. Below are links to PNe pretty-picture sites:

  • Hubble Space Telescope Gallery of Planetary Nebula Images

  • Bruce Balick's Planetary Nebula Gallery at SEDs.

  • George Jacoby's Planetary Nebula Sampler at NOAO.

Enough, already, back to the story...

Core Collapse to White Dwarf

The contracting C-O core becomes so dense that a new gas law takes over...

Degenerate Electron Gas:

  • Pressure becomes independent of Temperature
  • P grows rapidly & soon counteracts Gravity

Collapse halts when R ~ 0.01 Rsun (~ Rearth) Degenerate core becomes a White Dwarf

We will learn more about White Dwarfs in Unit 3. Return to [ Unit 2 Index | Astronomy 162 Main Page ] Updated: 2006 January 21 Copyright © Richard W. Pogge, All Rights Reserved.

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