• They follow very different paths when leaving the main sequence • The temperatures and densities in the cores are much different => different reactions HRD – massive stars Evolution – massive stars • They leave the main sequence when the hydrogen is depleted in their cores • The first few events are similar to those in lowermass stars: 1. hydrogen shell 2. core burning helium to carbon, surrounded by helium- and hydrogen-burning shells • Difference: stars with masses > 2.5 M have no helium flash but it starts gradually burning • It becomes a supergiant Evolution – massive stars • They undergo an extended sequence of thermonuclear reactions in its core and shells • These include carbon (12C) fusion, neon (20Ne) fusion, oxygen (16O) fusion, and silicon (28Si) fusion • See the slides in the lecture “Fusion – Fission” Evolution – core burning Evolution – massive stars Stage Core temperature (K) Core density (kg/m3) Duration of stage Hydrogen fusion 4 x 107 5 x 103 7 x 106 years Helium fusion 2 x 108 7 x 105 7 x 105 years Carbon fusion 6 x 108 2 x 108 600 years Neon fusion 1.2 x 109 4 x 109 1 year Oxygen fusion 1.5 x 109 1010 6 months Silicon fusion 2.7 x 109 3 x 1010 1 day Core collapse 5.4 x 109 3 x 1012 ¼ second Core bounce 2.3 x 1010 4 x 1015 milliseconds Explosive (Supernova) about 109 varies 10 seconds Stages for a star with 25 M • The last stage: 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 energy rather than causing energy to be released • Once the iron core is formed, the core contracts very rapidly and the temperature rises dramatically • Photodisintegration: high energy photons break the iron nuclei to helium nuclei • Electron combines with proton to form neutrons, neutrinos transport the energy • The core ends up as all neutron, with nuclear density (1017 kg/m3) • The degenerate neutron pressure suddenly halts the core contract • The outer core bounce back and sends a powerful wave of pressure • The pressure wave becomes a powerful shock wave as it go outwards, and expel most stellar material outward • Shock wave produces a series of nuclear reaction, the only place elements heavier than iron are produced in the universe Evolution – Supernova Supernova remnants X-ray Different Types of Supernovae • Type 1 supernova: no hydrogen lines – Type 1a supernova: explosion of white dwarf in a closed binary system; mass accumulation exceeds the critical mass and ignites the carbon fusion at the core – Type 1b supernova: core collapse of massive star with hydrogen shell lost before – Type 1c supernova: core collapse of massive star with both hydrogen and helium shells lost before • Type 2 supernova: strong hydrogen lines – core collapse of massive star with hydrogen shell largely intact Supernovae – classification scheme Type Ia supernovae are those produced by accreting white dwarfs in close binaries Type Ib supernovae occur when the star has lost a substantial part of its hydrogen shell Type Ic supernovae occur when the star has lost a substantial part of both its hydrogen shell and helium shell Type II supernovae are created by the deaths of massive stars Supernovae – light curves • Absolute magnitude is strongly correlated with rate of decline (faster = fainter) • Apply “stretch factor” to compensate for this Type Ia Supernovae as Standard Candles SN 1987A - the best observed SN • Occurred on 23.02.1987 • In the Large Magellanic Cloud reached V = 2.9 mag SN 1987A - the best observed SN • Progenitor star: blue B3 I supergiant SN 1987A: Neutrinos were detected • More than 99% of the energy from such a supernova is emitted in the form of neutrinos from the collapsing core • Neutrino energy 1046 Joules, 100 times as much energy as the Sun has emitted in its entire history • Neutrinos arrived 3 hours before the first SN light was seen • The 3-hour delay was due to the propagation time of the shock wave from the core to the surface of the supergiant SN 1987 A - the best observed SN SN 1987A - the best observed SN HST in 2017 SN 1987A - the best observed SN SN 1987A - the best observed SN