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Supernovae and nucleosynthesis of elements > Fe. Death of low-mass star: White Dwarf. White dwarfs are the remaining cores once fusion stops Electron degeneracy pressure supports them against gravity Cool and grow dimmer over time. A white dwarf can accrete mass from its companion. - PowerPoint PPT Presentation

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Page 1: Supernovae and nucleosynthesis of elements > Fe
Page 2: Supernovae and nucleosynthesis of elements > Fe

Supernovae and nucleosynthesis of elements > Fe

Page 3: Supernovae and nucleosynthesis of elements > Fe

Death of low-mass star: White Dwarf

• White dwarfs are the remaining cores once fusion stops

• Electron degeneracy pressure supports them against gravity

• Cool and grow dimmer over time

Page 4: Supernovae and nucleosynthesis of elements > Fe

A white dwarf can accrete mass from its companion

Page 5: Supernovae and nucleosynthesis of elements > Fe

Tycho’s supernova of 1572

Page 6: Supernovae and nucleosynthesis of elements > Fe

Expanding at 6 million mph

Page 7: Supernovae and nucleosynthesis of elements > Fe

Kepler’s supernova of 1609

Page 8: Supernovae and nucleosynthesis of elements > Fe

QuickTime™ and a decompressor

are needed to see this picture.

Supernovae outshine the

whole galaxy!

Page 9: Supernovae and nucleosynthesis of elements > Fe

Type I: White dwarf supernova

White dwarf near 1.4 Msun accretes matter from red giant companion, causing supernova explosion

Type II: Massive star supernova

Massive star builds up 1.4 Msun core and collapses into a neutron star, gravitational PE released in explosion

Two kinds of supernovae

Page 10: Supernovae and nucleosynthesis of elements > Fe

light curve shows how luminosity changes with time

Page 11: Supernovae and nucleosynthesis of elements > Fe

r process and s process elements

• Nuclear fusion in all stars only produces up to Fe-56• Slow neutron capture (s process) forms up to Bi-209 in

low-mass stars• High temps in SN creates elements up to Ca-254• Rapid neutron capture (r process) create neutron-rich

isotopes which decay into more stable neutron-rich elements

• Neutron flux during SN is 1022 neutrons per square centimeter per second

• neutron captures occur much faster than decays

Page 12: Supernovae and nucleosynthesis of elements > Fe

QuickTime™ and a decompressor

are needed to see this picture.

Page 13: Supernovae and nucleosynthesis of elements > Fe

A neutron star:

A few km in diameter, supported against gravity by degeneracy pressure of neutrons

Page 14: Supernovae and nucleosynthesis of elements > Fe

Discovery of Neutron Stars

• Using a radio telescope in 1967, Jocelyn Bell discovered very rapid pulses of radio emission coming from a single point on the sky

• The pulses were coming from a spinning neutron star—a pulsar

Page 15: Supernovae and nucleosynthesis of elements > Fe

Pulsar at center of Crab Nebula pulses 30 times per second

Page 16: Supernovae and nucleosynthesis of elements > Fe

Pulsars

Page 17: Supernovae and nucleosynthesis of elements > Fe

Thought Question

Could there be neutron stars that appear as pulsars to other civilizations but not to us?

A. YesB. No

Page 18: Supernovae and nucleosynthesis of elements > Fe

Thought Question

Could there be neutron stars that appear as pulsars to other civilizations but not to us?

A. YesB. No

Page 19: Supernovae and nucleosynthesis of elements > Fe

What happens if the neutron star has more mass than can be supported by neutron degeneracy pressure?

1. It will collapse further and become a black hole

2. It will spin even faster, and fling material out into space

3. Neutron degeneracy pressure can never be overcome by gravity

Page 20: Supernovae and nucleosynthesis of elements > Fe

• Neutron degeneracy pressure can no longer support a neutron star against gravity if its mass is > about 3 Msun

Page 21: Supernovae and nucleosynthesis of elements > Fe

18.3 Black Holes: Gravity’s Ultimate Victory

A black hole is an object whose gravity is so powerful that not even light can escape it.

Page 22: Supernovae and nucleosynthesis of elements > Fe

Escape Velocity

Initial KineticEnergy

Final Gravitational Potential Energy

=

1

2mv 2 =

GmM

r

Where m is your mass, M is the mass of the object that you are trying to escape from, andr is your distance from that object

Page 23: Supernovae and nucleosynthesis of elements > Fe

Light would not be able to escape Earth’s surface if you could shrink it to < 1 cm

Page 24: Supernovae and nucleosynthesis of elements > Fe

“Surface” of a Black Hole

• The “surface” of a black hole is the distance at which the escape velocity equals the speed of light.

• This spherical surface = event horizon.

• The radius of the event horizon is known as the Schwarzschild radius.

Page 25: Supernovae and nucleosynthesis of elements > Fe

The event horizon of a 3 MSun black hole is a few km

Neutron star

Page 26: Supernovae and nucleosynthesis of elements > Fe

A black hole’s mass strongly warps space and time in vicinity of event horizon

Page 27: Supernovae and nucleosynthesis of elements > Fe

What would it be like to visit a black hole?

Page 28: Supernovae and nucleosynthesis of elements > Fe

Light waves take extra time to climb out of a deep hole in spacetime, leading to a gravitational redshift

Page 29: Supernovae and nucleosynthesis of elements > Fe

Time passes more slowly near the event horizon

Page 30: Supernovae and nucleosynthesis of elements > Fe

Thought Question

Is it easy or hard to fall into a black hole?

A. EasyB. Hard

Page 31: Supernovae and nucleosynthesis of elements > Fe

Tidal forces near the event horizon of a 3 MSun black hole would be lethal to humans

Tidal forces would be gentler near a supermassive black hole because its radius is much bigger

Page 32: Supernovae and nucleosynthesis of elements > Fe

Do black holes really exist?

Page 33: Supernovae and nucleosynthesis of elements > Fe

Black Hole Verification

• Need to measure mass— Use orbital properties of companion— Measure velocity and distance of orbiting gas

• It’s a black hole if it’s not a star and its mass exceeds the neutron star limit (~3 MSun)

Page 34: Supernovae and nucleosynthesis of elements > Fe

Some X-ray binaries contain compact objects of mass exceeding 3 MSun which are likely to be black holes

Page 35: Supernovae and nucleosynthesis of elements > Fe

One famous X-ray binary with a likely black hole is in the constellation Cygnus

Page 36: Supernovae and nucleosynthesis of elements > Fe

Thought Question

How does the radius of the event horizon change when you add mass to a black hole?

A. IncreasesB. DecreasesC. Stays the same

Page 37: Supernovae and nucleosynthesis of elements > Fe

Thought Question

How does the radius of the event horizon change when you add mass to a black hole?

A. IncreasesB. DecreasesC. Stays the same

Page 38: Supernovae and nucleosynthesis of elements > Fe

Thought Question

Is it easy or hard to fall into a black hole?

A. EasyB. Hard

Hint: A black hole with the same mass as the Sun wouldn’t be much bigger than a college campus

Page 39: Supernovae and nucleosynthesis of elements > Fe

Thought Question

Is it easy or hard to fall into a black hole?

A. EasyB. Hard

Hint: A black hole with the same mass as the Sun wouldn’t be much bigger than a college campus

Page 40: Supernovae and nucleosynthesis of elements > Fe

If the Sun shrank into a black hole, its gravity would be different only near the event horizon

Black holes don’t suck!

Page 41: Supernovae and nucleosynthesis of elements > Fe

Event horizon is larger for black holes of larger mass

Black holes have only mass, spin and charge