astr100 (spring 2008) introduction to astronomy life as a low-mass star prof. d.c. richardson...

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ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

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Page 1: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

ASTR100 (Spring 2008) Introduction to AstronomyLife as a Low-mass Star

Prof. D.C. Richardson

Sections 0101-0106

Page 2: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

What are the life stages of a low-mass star?

Page 3: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

A star remains on the main sequence as long as it can fuse hydrogen into helium in its core.

Page 4: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

What happens when a star can no longer fuse hydrogen to helium in its core?

A.Core cools off.B.Core shrinks and heats up.C.Core expands and heats up.D.Helium fusion begins immediately.

Page 5: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

What happens when a star can no longer fuse hydrogen to helium in its core?

A.Core cools off.B.Core shrinks and heats up.C.Core expands and heats up.D.Helium fusion begins immediately.

Page 6: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Life Track After Main Sequence

Observations of star clusters show star becomes larger, redder, and more luminous after its time on the main sequence is over.

Page 7: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Broken Thermostat

As core contracts, H begins fusing to He in a shell around core.

Luminosity rises because core thermostat broken: increasing fusion rate in shell does not stop core from contracting.

Page 8: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

He-fusion requires higher temperatures than H-fusion because larger charge leads to greater repulsion.

Fusion of two He nuclei doesn’t work, so He-fusion must combine three He nuclei to make carbon (C).

Page 9: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

What happens in a low-mass star when core temperature rises enough for helium fusion to begin?

A.Helium fusion slowly starts up.B.Hydrogen fusion stops.C.Helium fusion rises very rapidly.

Hint: degeneracy pressure is the main form of pressure in the inert helium core.

Page 10: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

What happens in a low-mass star when core temperature rises enough for helium fusion to begin?

A.Helium fusion slowly starts up.B.Hydrogen fusion stops.C.Helium fusion rises very rapidly.

Page 11: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Helium Flash

Thermostat broken in low-mass red giant because degeneracy pressure supports core.

Core temperature rises rapidly when helium fusion begins.

Helium fusion rate skyrockets until thermal pressure takes over and expands core again.

Page 12: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Helium-burning stars neither shrink nor grow because thermostat is temporarily fixed.

Page 13: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Life Track After Helium Flash

Models show that a red giant should shrink and become less luminous after helium fusion begins in the core.

Page 14: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Life Track After Helium Flash

Observations of star clusters agree with those models.

Helium-burning stars are found in a horizontal branch on the H-R diagram.

Page 15: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

How does a low-mass star die?

Page 16: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

What happens when a star’s core runs out of helium?

A.The star explodes.B.Carbon fusion begins.C.The core cools off.D.Helium fuses in a shell around the

core.

Page 17: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

What happens when a star’s core runs out of helium?

A.The star explodes.B.Carbon fusion begins.C.The core cools off.D.Helium fuses in a shell around the

core.

Page 18: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Double Shell Burning

Late in its life, a star like our Sun will have… An inert carbon core… …surrounded by a shell of fusing helium… …surrounded by a shell of fusing hydrogen.

The star swells enormously in size, even bigger than before.

But the core never gets hot enough to fuse carbon.

Page 19: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

A star like our sun dies by puffing off its outer layers, creating a planetary nebula.

Only a white dwarf is left behind.

Page 20: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

A star like our sun dies by puffing off its outer layers, creating a planetary nebula.

Only a white dwarf is left behind.

Page 21: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

A star like our sun dies by puffing off its outer layers, creating a planetary nebula.

Only a white dwarf is left behind.

Page 22: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

A star like our sun dies by puffing off its outer layers, creating a planetary nebula.

Only a white dwarf is left behind.

Page 23: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Helix Nebula

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 24: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Cat’s Eye Nebula

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 25: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

White Dwarf

No fusion, and it cannot contract (due to degeneracy pressure).

So a white dwarf just cools off forever, fading away…

Page 26: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Life stages of a low-mass star like the Sun.

Page 27: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Life Track of a Sun-like Star

Page 28: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

ASTR100 (Spring 2008) Introduction to AstronomyLife as a High-mass Star

Prof. D.C. Richardson

Sections 0101-0106

Page 29: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

What are the life stages of a high-mass star?

Page 30: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

CNO Cycle

High-mass main- sequence stars fuse H to He at a higher rate using carbon, nitrogen, and oxygen as catalysts.

A greater core temperature enables H nuclei to overcome greater repulsion.

Page 31: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Life Stages of High-mass Stars

Late life stages of high-mass stars are similar to those of low-mass stars… Hydrogen core fusion (main sequence). Hydrogen shell burning (supergiant). Helium core fusion (supergiant).

Page 32: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

How do high-mass stars make the elements necessary for

life?

Page 33: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Big Bang made 75% H, 25% He — stars make everything else.

Page 34: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Helium fusion can make carbon in low-mass stars.

Page 35: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

CNO cycle in high-mass stars can change C N & O.

Page 36: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Helium Capture

High core temperatures allow helium to fuse with heavier elements.

Page 37: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Helium capture builds C into O, Ne, Mg, …

Page 38: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Advanced Nuclear Burning

Core temperatures in stars > 8 MSun allow fusion of elements as heavy as iron.

Page 39: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Advanced reactions in stars make elements like Si, S, Ca, and Fe.

Page 40: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

The Death Sequence of a High-Mass Star

Multiple-Shell Burning

Advanced nuclear burning proceeds in a series of nested shells.

Page 41: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Iron is a dead end for fusion because nuclear reactions involving iron do not release energy.

(Fe has lowest mass per nuclear particle.)

Page 42: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Evidence for helium capture:

Higher abundances of elements with even numbers of protons.

Page 43: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

How does a high-mass star die?

Page 44: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Iron builds up in core until degeneracy pressure can no longer resist gravity.

Core then suddenly collapses, creating supernova explosion.

Page 45: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Supernova Simulation

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Page 46: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Supernova Explosion

Core degeneracy pressure goes away because electrons combine with protons, making neutrons and neutrinos.

Neutrons collapse to the center, forming a neutron star.

Page 47: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Energy and neutrons released in supernova explosion enable elements heavier than iron to form, e.g. Au, U.

Page 48: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Elements made during supernova explosions.

Page 49: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Multiwavelength Crab Nebula

Supernova Remnant

Energy released by the collapse of the core drives outer layers into space.

The Crab Nebula is the remnant of the supernova seen in A.D. 1054.

Page 50: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Supernova 1987A

The closest supernova in the last four centuries was seen in 1987.

Page 51: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

The next nearby supernova?

Page 52: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

How does a star’s mass determine its life story?

Page 53: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Role of Mass

A star’s mass determines its entire life story because it determines its core temperature.

High-mass stars have short lives, eventually becoming hot enough to make iron, and end in supernova explosions.

Low-mass stars have long lives, never becoming hot enough to fuse carbon nuclei, and end as white dwarfs.

Page 54: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Low-mass Star Summary

1. Main Sequence: H fuses to He in core.

2. Red Giant: H fuses to He in shell around He core.

3. Helium Core Burning: He fuses to C in core while H fuses to He in shell.

4. Double Shell Burning: H and He both fuse in shells.

5. Planetary Nebula leaves White Dwarf behind.

Not to scale!

Page 55: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Reasons for Life Stages

Core shrinks and heats until it’s hot enough for fusion.

Nuclei with larger charge require higher temperature for fusion.

Core thermostat is broken while core is not hot enough for fusion (shell burning).

Core fusion can’t happen if degeneracy pressure keeps core from shrinking.

Not to scale!

Page 56: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

High-mass Star Summary

1. Main Sequence: H fuses to He in core.

2. Red Supergiant: H fuses to He in shell around He core.

3. Helium Core Burning: He fuses to C in core while H fuses to He in shell.

4. Multiple Shell Burning: Many elements fuse in shells.

5. Supernova leaves Neutron Star behind.

Not to scale!

Page 57: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

How are the lives of stars with close companions

different?

Page 58: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Thought Question

The binary star Algol consists of a 3.7 MSun main-sequence star and a 0.8 MSun subgiant star…

What’s strange about this pairing?

How did it come about?

Page 59: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

Stars in Algol are close enough that matter can flow from the subgiant onto the main-sequence star.

Page 60: ASTR100 (Spring 2008) Introduction to Astronomy Life as a Low-mass Star Prof. D.C. Richardson Sections 0101-0106

The star that is now a subgiant was originally more massive.

As it reached the end of its life and started to grow, it began to transfer mass to its companion (mass exchange).

Now the companion star is more massive.