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Supernova

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Once high mass stars are off the main sequence, they have different post MS ... High mass stars burn many elements and have 'onion-like' shells of material ... – PowerPoint PPT presentation

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Title: Supernova


1
Supernova
  • Physical Astronomy
  • Professor Lee Carkner
  • Lecture 17

2
High Mass Stars
  • Very high mass stars (Mgt8Msun) are rare and also
    can have extreme properties
  • Have rapid, dramatic post main sequence evolution
  • Go supernova
  • producing very heavy elements

3
Luminous Blue Variables
  • T 15000-30000 K, L 106 Lsun
  • Occupy an instability zone on the HR diagram
  • What accounts for mass loss and variability?
  • Pulsation

4
Wolf-Rayet Stars
  • Hot, bright stars with rapid rotation and mass
    loss
  • Have strong emissions lines of different elements
  • WN He and N
  • WC He and C
  • WO O
  • from C He burning

5
High Mass Evolution
  • Once high mass stars are off the main sequence,
    they have different post MS stages than low mass
    stars
  • Then a Wolfe-Rayet stage
  • Ends life with supernova

6
Types of Supernovae
  • Nova just means new star
  • A supernova is a very bright nova
  • Accretion onto white dwarf causing core collapse
    (Type Ia)
  • Core collapse of high mass star (Type Ib, Ic, and
    II)

7
Classification
  • Supernovae classified by spectral features and
    light curve
  • Must be from stars that have lost their outer
    layers
  • Type Ib have strong He
  • Type II have strong H
  • Type II-L have a more rapid drop off

8
Core Collapse
  • Excluding the Type Ia, we can refer to the rest
    as core collapse supernova
  • Generates about 1046 J of energy
  • mostly in the form of neutrinos

9
The Core
  • High mass stars burn many elements and have
    onion-like shells of material
  • As the fusion products move towards iron, the
    energy released per nuclei decreases
  • Iron cant be burned, so star cant stay in HSE

10
Core Processes
  • The iron burning core is so hot the photons have
    enough energy to destroy nuclei
  • T and P are also high enough that the protons can
    fuse with electrons, producing neutrons
  • Cores ability to support outer layers drops
    rapidly
  • Removing electrons decreases electron degeneracy
    pressure

11
Explosion
  • We can try to model supernova on computers
  • hard to do
  • This causes the collapse to rebound and send a
    shock wave out
  • A neutrinosphere forms behind the shock
  • Blasts atmosphere away and produces 1036 W of
    radiation
  • about billion suns

12
Supernova 1987A
  • Located in Milky Way satellite the Large
    Magellanic Cloud
  • Progenitor was 12th magnitude blue supergiant

13
End Products
  • If initial star was smaller than about 35 Msun,
    core will form a neutron star
  • Remains of atmosphere and shock wave form
    supernova remnant
  • Remnant can also collide with ISM causing
    emission and triggering star formation

14
Radioactive Decay
  • The decay of these isotopes add energy to the
    supernova and effect the shape of the light curve
  • Most important reaction is 56Ni decaying to 56Co
    and then 56Fe
  • With half life of 6.1 days and 77.7 days

15
Half-Life
  • How much energy is released by decay?
  • Decay goes as
  • N(t) N0e-lt
  • Where N0 is the initial number of atoms and N is
    the number at some time t
  • l (ln 2)/t1/2
  • where t1/2 is the half-life (time for ½ of atoms
    to decay)

16
Light Curve Slope
  • The magnitude of the supernova is proportional to
    l
  • dMbol/dt 1.086l
  • For example supernova 1987A has a light curve
    after 200 days well matched by 56Co and 57Co

17
Elemental Abundances
  • H and He are the most plentiful
  • Li, Be, B underabundant
  • Some elements (C, O, Ne, ) are abundant because
    the are created in post-main sequence stars
  • Fe created in supernovae cores

18
Next Time
  • Test 2
  • Same structure as test 1
  • 8 multiple choice, 4 problems
  • For Friday
  • Read 16.1-16.5
  • Homework 16.1b,c,d, 16.4
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