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The Deaths of Stars 1 Guiding Questions 1 What kinds of nuclear reactions occur within a star like the Sun as it ages 2 Where did the carbon atoms in our bodies come from 3 What is a planetary nebula and what does it have to do with planets 4 What is a white dwarf star 5 Why do high mass stars go through more evolutionary stages than low mass stars 6 What happens within a high mass star to turn it into a supernova 7 Why was SN 1987A an unusual supernova 8 What was learned by detecting neutrinos from SN 1987A 9 How can a white dwarf star give rise to a type of supernova 10 What remains after a supernova explosion 2 Pathways of Stellar Evolution GOOD TO KNOW 3 Low mass stars go through two distinct red giant stages A low mass star becomes a red giant when shell hydrogen fusion begins a horizontal branch star when core helium fusion begins an asymptotic giant branch AGB star when the helium in the core is exhausted and shell helium fusion 4 begins 5 6 7 Bringing the products of nuclear fusion to a giant star s surface As a low mass star ages convection occurs over a larger portion of its volume This takes heavy elements formed in the star s interior and distributes them throughout the star 8 9 Low mass stars die by gently ejecting their outer layers creating planetary nebulae Helium shell flashes in an old low mass star produce thermal pulses during which more than half the star s mass may be ejected into space This exposes the hot carbon oxygen core of the star Ultraviolet radiation from the exposed core ionizes and excites the ejected gases producing a planetary nebula 10 11 12 13 14 Why do planetary nebulae look so different from one another 15 The burned out core of a low mass star cools and contracts until it becomes a white dwarf No further nuclear reactions take place within the exposed core Instead it becomes a degenerate dense sphere about the size of the Earth and is called a white dwarf It glows from thermal radiation as the sphere cools it becomes dimmer 16 17 18 19 High mass stars create heavy elements in their cores Unlike a low mass star a high mass star undergoes an extended sequence of thermonuclear reactions in its core and shells These include carbon fusion neon fusion oxygen fusion and silicon fusion 20 21 In the last stages of its life a high mass star has an iron rich core surrounded by concentric shells hosting the various thermonuclear reactions The sequence of thermonuclear reactions stops here because the formation of elements heavier than iron requires an input of 22 energy rather than causing energy to be released High mass stars violently blow apart in supernova explosions A high mass star dies in a violent cataclysm in which its core collapses and most of its matter is ejected into space at high speeds The luminosity of the star increases suddenly by a factor of around 108 during this explosion producing a supernova The matter ejected from the supernova moving at supersonic speeds through interstellar gases and dust glows as a nebula called a supernova remnant 23 24 25 In 1987 a nearby supernova gave us a close up look at the death of a massive star 26 27 28 Neutrinos emanate from supernovae like SN 1987A More than 99 of the energy from such a supernova is emitted 29 in the form of neutrinos from the collapsing core White dwarfs in close binary systems can also become supernovae An accreting white dwarf in a close binary system may become a supernova when carbon fusion ignites explosively throughout the degenerate star 30 Type Ia supernovae are those produced by accreting white dwarfs in close binaries 31 Type Ib and Type Ic supernovae occur when the star has lost a substantial part of its outer layers before exploding 32 33 Type II supernovae are created by the deaths of massive stars 34 35 Most supernovae occurring in our Galaxy are hidden from our view by interstellar dust and gases but a supernova remnant can be detected at many wavelengths for centuries after the explosion 36 Jargon asymptotic giant branch asymptotic giant branch star AGB star carbon fusion carbon star Cerenkov radiation Chandrasekhar limit core helium fusion dredge up helium shell flash horizontal branch mass radius relation neon fusion neutron capture nuclear density oxygen fusion photodisintegration planetary nebula progenitor star red giant branch shell helium fusion silicon fusion supergiant supernova plural supernovae supernova remnant thermal pulse Type I supernova Type Ia supernova Type Ib supernova Type Ic supernova Type II supernova white dwarf 37


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MASON ASTR 113 - The Deaths of Stars

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