A nova is a star that brightens suddenly by 100 to 10,000 times in a single day.
![]() |
Novae are frequently (perhaps always) members of binary systems where the more massive star evolves more quickly and becomes a white dwarf. The less massive star loses some of its hydrogen-rich outer atmosphere to the white dwarf where it collects. (adapted by G. Rieke from J. Blondin, http://wonka.physics.ncsu.edu/~blondin/AAS/) |
![]() |
The high gravity and intense heat of the white dwarf make conditions suitable for hydrogen fusion into helium. When enough hydrogen collects, it explodes in a fusion reaction, causing a nova. The gas ejected in the explosion is moving outwards at 1000-2000 kms/sec. (adapted by G. Rieke from HEASARC) |
are stars that end their lifetimes in a violent
nuclear explosion during which a single star can become as bright as
an entire galaxy like the Milky Way. When one explodes nearby, the appearance of a bright
new star is an awesome sight
| Two Types of Supernovae
By examining both the light curves and spectra of supernovae, we have learned that there are two very different causes for a supernova explosion.
from J. Kaler via http://www.chapman.edu/oca/benet/intro_sn.htm
|
![]() |
Type I:
![]() |
The "Type I" supernovae arise
when the white dwarf star member of a binary system accretes so much matter from its
companion that it is tipped over the 1.4M |
Type II:
![]() |
The "Type II" supernovae are the
result of a massive star consuming all of its nuclear fuel and then exploding. The black
line traces the evolution of a massive star schematically, until it reaches the supernova
stage. (from G. Smith, http://casswww.ucsd.edu/public/tutorial/SN.html)
|
![]() |
This figure (from The Essential Cosmic
Perspective, Bennett et al.) shows how the greatest binding energy
per nuclear particle occurs for iron. Thus, when the stellar core becomes solid iron, there is no reaction available to produce energy to keep the core hot and maintain the pressure that resists gravity; the iron core collapses in just a few seconds to a neutron star (or black hole). |
Core Collapse and Supernovae
With the support from the core removed, the upper layers of the star collapse. When they hit the new, very hard neutron-star core, they bounce and send material crashing back up through the still-falling layers (see simulation below). The result is a rapid increase in temperature to several billions of degrees.
![]() |
This simulation shows what happens in the upper layers of the star as the shock passes through them. The neutron star core is at the lower left corner. The huge release of energy causes much of the hydrogen to fuse into helium, releasing huge amounts of energy that create the visible supernova. So much energy is released that the material in the star can react and produce all the elements heavier than iron, none of which can be produced during the previous life of the star. Animation from Tetsuya Shimizu. |
![]() |
Here is a more distant overview of the process |
![]() |
And how it might look from a desolate planet orbiting the star, with the optimistic assumption that the observer would live long enough to see the pulsar emerge! Animation from NASA/HEASARC |
After collapse, the stellar brightness increases dramatically (by a least at factor of 10,000)
In the end, all the outer layers of the star are blown away, leaving only a black hole or neutron star -- the latter may send out searchlight beams of light that sweep the sky as it spins and can appear to us as a pulsar.
The properties of a Type I explosion differ from a Type II because the white dwarf never synthesized any elements heavier than carbon in its core.
What becomes of any core material left from a supernova explosion?
1) If the core which remains has a mass <~3M
, it will
become a neutron star/pulsar like the Crab pulsar.
2) If the core is too massive, it will become a black hole because not even neutron degeneracy pressure will be able to resist the force of gravity.
Test your understanding before going on![]()
![]()
"Embedding" diagram, showing how a black hole distorts space/time, from C. Pickover, http://sprott.physics.wisc.edu/pickover/graphcp.html |
![]()
Anasazi painting of Crab supernova, Canyon de Chelly, http://www.colorado.edu/Conferences/chaco/tour/blanco.htm |
|
Click to return to syllabus |
||
| Click to return to Stellar Black Holes | hypertext © G. H. Rieke |
Click to go to Supernova Remnants |