chapter 21 stellar explosions

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Chapter 21 Stellar Explosions

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Chapter 21 Stellar Explosions. Units of Chapter 21. 21.1Life after Death for White Dwarfs 21.2The End of a High-Mass Star 21.3Supernovae Supernova 1987A 21.4The Formation of the Elements 21.5The Cycle of Stellar Evolution. 21.1 Life after Death for White Dwarfs. - PowerPoint PPT Presentation

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Page 1: Chapter 21 Stellar Explosions

Chapter 21 Stellar Explosions

Page 2: Chapter 21 Stellar Explosions

21.1 Life after Death for White Dwarfs21.2 The End of a High-Mass Star21.3 Supernovae

Supernova 1987A21.4 The Formation of the Elements21.5 The Cycle of Stellar Evolution

Units of Chapter 21

Page 3: Chapter 21 Stellar Explosions

A nova is a star that flares up very suddenly and then returns slowly to its former luminosity:

21.1 Life after Death for White Dwarfs

Page 4: Chapter 21 Stellar Explosions

A white dwarf that is part of a semidetached binary system can undergo repeated novas.

Page 5: Chapter 21 Stellar Explosions

Material falls onto the white dwarf from its main-sequence companion. When enough material has accreted, fusion can reignite very suddenly, burning off the new material. Material keeps being transferred to the white dwarf, and the process repeats, as illustrated here:

Page 6: Chapter 21 Stellar Explosions

This series of images shows ejected material expanding away from a star after a nova explosion:

Page 7: Chapter 21 Stellar Explosions

A high-mass star can continue to fuse elements in its core right up to iron (after which the fusion reaction is energetically unfavored).As heavier elements are fused, the reactions go faster and the stage is over more quickly. A 20-solar-mass star will burn carbon for about 10,000 years, but its iron core lasts less than a day.

21.2 The End of a High-Mass Star

Page 8: Chapter 21 Stellar Explosions

This graph shows the relative stability of nuclei. On the left, nuclei gain energy through fusion; on the right they gain it through fission:

Iron is the crossing point; when the core has fused to iron, no more fusion can take place

Page 9: Chapter 21 Stellar Explosions

The inward pressure is enormous, due to the high mass of the star.There is nothing stopping the star from collapsing further; it does so very rapidly, in a giant implosion.As it continues to become more and more dense, the protons and electrons react with one another to become neutrons:

p + e → n + neutrino

Page 10: Chapter 21 Stellar Explosions

The neutrinos escape; the neutrons are compressed together until the whole star has the density of an atomic nucleus, about 1015 kg/m3.The collapse is still going on; it compresses the neutrons further until they recoil in an enormous explosion as a supernova.

Page 11: Chapter 21 Stellar Explosions

A supernova is incredibly luminous—as can be seen from these curves—and more than a million times as bright as a nova:

21.3 Supernovae

Page 12: Chapter 21 Stellar Explosions

A supernova is a one-time event—once it happens, there is little or nothing left of the progenitor star.There are two different types of supernovae, both equally common:

•Type I, which is a carbon-detonation supernova, and•Type II, which is the death of a high-mass star just

described

Page 13: Chapter 21 Stellar Explosions

Carbon-detonation supernova: white dwarf that has accumulated too much mass from binary companionIf the white dwarf’s mass exceeds 1.4 solar masses, electron degeneracy can no longer keep the core from collapsing.Carbon fusion begins throughout the star almost simultaneously, resulting in a carbon explosion.

Page 14: Chapter 21 Stellar Explosions

This graphic illustrates the two different types of supernovae:

Page 15: Chapter 21 Stellar Explosions

Supernovae leave remnants—the expanding clouds of material from the explosion. The Crab nebula is a remnant from a supernova explosion that occurred in the year 1054.

Page 16: Chapter 21 Stellar Explosions

The velocities of the material in the Crab nebula can be extrapolated back, using Doppler shifts, to the original explosion.

Page 17: Chapter 21 Stellar Explosions

This is the Vela supernova remnant: Extrapolation shows it exploded about 9000 BCE

Page 18: Chapter 21 Stellar Explosions

Supernovae are rare; there has not been one in our galaxy for about 400 years.A supernova, called SN1987A, did occur in the Large Magellanic Cloud, a neighboring galaxy, in 1987. Its light curve is somewhat atypical:

Discovery 21-1: Supernova 1987A

Page 19: Chapter 21 Stellar Explosions

A cloud of glowing gas is now visible around SN1987A, and a small central object is becoming discernible:

Discovery 21-1: Supernova 1987A

Page 20: Chapter 21 Stellar Explosions

There are 81 stable and 10 radioactive elements that exist on our planet. Where did they come from?

This graph shows the relative abundances of different elements in the universe:

21.4 The Formation of the Elements

Page 21: Chapter 21 Stellar Explosions

Some of these elements are formed during normal stellar fusion. Here, three helium nuclei fuse to form carbon:

Page 22: Chapter 21 Stellar Explosions

Carbon can then fuse, either with itself or with alpha particles, to form more nuclei:

Page 23: Chapter 21 Stellar Explosions

The elements that can be formed through successive alpha-particle fusion are more abundant than those created by other fusion reactions:

Page 24: Chapter 21 Stellar Explosions

The last nucleus in the alpha-particle chain is nickel-56, which is unstable and quickly decays to cobalt-56 and then to iron-56.Iron-56 is the most stable nucleus, so it neither fuses nor decays.However, within the cores of the most massive stars, neutron capture can create heavier elements, all the way up to bismuth-209.The heaviest elements are made during the first few seconds of a supernova explosion.

Page 25: Chapter 21 Stellar Explosions

This theory of formation of new elements in supernova explosions produces a light curve that agrees quite well with observed curves:

Page 26: Chapter 21 Stellar Explosions

Star formation is cyclical: Stars form, evolve, and die.In dying, they send heavy elements into the interstellar medium.These elements then become parts of new stars.And so it goes.

21.5 The Cycle of Stellar Evolution

Page 27: Chapter 21 Stellar Explosions

After a star's core runs out of fuel, how does the core get to a high enough temperature to ignite the next stage of fusion reactions? A. By chemical reactions.B. By other fusion reactions.C. By gravitational contraction.D. None of these; the fusion reactions

stop.

Page 28: Chapter 21 Stellar Explosions

The kinds of thermonuclear reactions that will eventually occur in the core of a star depends on its

A. mass.B. radius.C. Doppler shift.D. abundance of carbon atoms

when it formed.

Page 29: Chapter 21 Stellar Explosions

One of the causes for the phenomenon called a nova is A. the fusion of iron in the core of a

massive star.B. the in fall of material onto a neutron

star from a white dwarf.C. the transfer of material onto a white

dwarf in a double star system.D. the collapse of a proto star.E. the death of a massive star and the

formation of a black hole.

Page 30: Chapter 21 Stellar Explosions

When a star dies, it becomes a supernova

A. Always.B. only if it is a few times more

massive than the sun.C. only if it includes the whole

galaxy.D. Never.

Page 31: Chapter 21 Stellar Explosions

Type I supernovae are produced:

A. when a high mass star gets to the iron fusion limit.

B. when a star reaches the Chandrasekhar limit.

C. as the result of fusionable material being accreted by a white dwarf star from its binary companion.

D. as a result of the helium flash in a 4 to 5 solar mass star.

Page 32: Chapter 21 Stellar Explosions

The crab nebula is

A. a supernova remnant.

B. a newly forming star.

C. an h-2 region.D. a black hole

Page 33: Chapter 21 Stellar Explosions

How are elements with nuclei heavier than iron produced? A. They are produced in the same way as

lighter elements by fusion of helium nuclei with heavier nuclei.

B. They are produced during supernova explosions.

C. They are produced by the interaction of the interstellar medium with material of planetary nebulae.

D. They are produced by mass accretion of one member of a binary star from the other member.

Page 34: Chapter 21 Stellar Explosions

An object of which of the following categories has the least density?

A. Main sequence stars.B. Nebulae.C. Pulsars.D. Red giants.E. White dwarfs.

Page 35: Chapter 21 Stellar Explosions

Stars which contribute most to the chemical enrichment of the interstellar medium are stars which are

A. less massive than the sun.B. solar mass stars.C. more massive than the sun.D. none of the above; stars do not

enrich the interstellar medium, galaxies do.

Page 36: Chapter 21 Stellar Explosions

• A nova is a star that suddenly brightens and gradually fades; it is a white dwarf whose larger partner continually transfers material to it.• Stars greater than eight solar masses can have fusion in their cores going all the way up to iron, which is stable against further fusion.• The star continues to collapse after the iron core is found, implodes, and then explodes as a supernova.

Summary of Chapter 21

Page 37: Chapter 21 Stellar Explosions

•Two types of supernovae:

•All elements heavier than helium are formed in stars:

Summary of Chapter 21 (cont.)

• Type I, a carbon-detonation supernova• Type II, a core-collapse supernova

• Elements up to bismuth-209 are formed in stellar cores during fusion• Heavier elements are created during supernova explosions