Astro 1 - Lecture 25


Matthew A. Bershady

Department of Astronomy & Astrophysics

Penn State University


Fall 1996

This document may not be copied for sale

All Rights Reserved

© 1995 Matthew A. Bershady

Lectures Lecture page Astro1 page



END GAME I: EXPLOSION



1. The importance of star clusters


Times scales for different stages of stellar evolution ...

How can we check?

(i) Observe HR diagrams for clusters

(ii) Measure relative density of stars at different stages

(iii) Combine information for many clusters of different ages


assumption:

The number of stars as a function of mass is constant over a small range of mass


So what are those ``blue stragglers?''




2. Binaries and Mass Transfer: Stellar Thieves


Mass from one star gravitationally 'stolen' by companion:



Nova:

surface-fusion of Hydrogen on a white dwarf

(non-destructive for white dwarf)

Super-nova:

catastrophic explosion


Nova vs. Super-nova:

- different light curves

- different amounts of energy released




3. High Mass Stellar Evolution


Short lives

Heavy element production in ``onion skin'' layers of star

- off the Main Sequence

The most massive stars ``burn'' up to iron in the core

Iron is the ``limit'' for exothermic fusion

- i.e., iron cannot fuse with anything to produce energy

- iron nuclei are the most stable of heavy elements


So what happens after the iron core is formed ?


uh oh ...




4. Core Collapse


. . . beyond white dwarf densities


Here's the scenario:


(a) Collapse heats core

(b) Nuclei are broken apart n, p+

+ all the e- already there

= hot, dense particle soup

(c) electrons (e-) more and more degenerate

(d) protons (p+) and neutrons (n) also degenerate,

- but not as much as e-:

``Fermi Sea'' isn't as high

Why: They are not fundamental particles

More states per given energy level

(e) Electron ``Fermi Energy'' high enough for e- to form heavier particles:

e- + p+ n +

`` inverse beta decay ''

(f) e- degeneracy decreases

(g) n degeneracy increases

(h) collapse comes to ``screeching'' halt

(i) core bounces

(j) shock wave rips apart outer layers of star


Super-nova explosion (Type II)




5. Super novae types


Two types:

Type I

observed: Hydrogen poor

white-dwarfs ``over the limit'' (mass limit)

explosive Carbon fusion in core

``Carbon Flash'' - a deflagration

entire star is ripped apart

Type II

observed: Hydrogen rich

massive stars with iron cores

core bounce

formation of a neutron star


Type I mass limit: white dwarf ``critical mass''

Nobel prize winner

Died: 1995

Over this mass, white-dwarf core collapses;

electron degeneracy pressure overwhelmed by gravity.




Q25.1 How does the increase of electron degeneracy in a collapsing iron core lead to the formation of a neutron star?

(a) the electron Fermi Energy becomes high enough for electrons and protons to form neutrons

(b) the neutron Fermi Sea compresses the electrons into the protons

(c) degeneracy is a state where one particle transforms into another particle

(d) the iron nuclei in the core interact with the electrons, and transform them into neutrons

(e) as the iron nuclei are ripped apart, this forces the electrons to become more degenerate


Q25.2 What is not a difference between Type I and Type II supernovae?

(a) stellar progenitors

(b) composition

(c) light curves

(d) remnants

(e) brighter than a nova


Lectures Lecture page Astro1 page

This page and its links look best with Netscape 2.0 image options set to "dither."

Last updated: Oct 11, 1996 Matthew A. Bershady