Planetary Nebulae are the remnants of stars with 1 Msun to a few Msun, with radii from 0.2 to 3 light years, expanding at 10 to 20 km/s, and their phase lasts less than 10,000 years.
Planetary Nebulae have nothing to do with planets.
The formation of Planetary Nebulae involves a two-stage process: a slow wind from a red giant blows away cool, outer layers of the star, and a fast wind from hot, inner layers of the star overtakes the slow wind and excites it, forming a Planetary Nebula.
White Dwarfs are degenerate stellar remnants with a C,O core, extremely dense, and a mass of 1 teaspoon of material would weigh 16 tons.
White dwarfs have a mass of ~1 solar mass, a temperature of 25,000 K, and a luminosity of 0.01 Lsun.
A chunk of white dwarf material the size of a beach ball would outweigh an ocean liner.
White dwarfs are found in the lower center/left of the Herzsprung-Russell diagram due to their low luminosity and high temperature.
The Chandrasekhar Limit states that the more massive a white dwarf, the smaller it is, until electron degeneracy pressure can no longer hold it up against gravity.
In a binary system, each star controls a finite region of space, bounded by the Roche Lobes (or Roche surfaces).
Lagrange points are points of stability, where matter can remain without being pulled towards one of the stars.
Matter can flow over from one star to another through the Inner Lagrange Point, L1.
Mass transfer in a binary system can significantly alter the stars’ masses and affect their stellar evolution.
In a binary system consisting of a white dwarf and a main sequence or red giant star, the white dwarf accretes matter from the companion.
Angular momentum conservation in a binary system means that the accreted matter forms a disk, called an accretion disk.
Matter in the accretion disk heats up to ~1 million K, resulting in X-ray emission, which is an “X-ray binary”.
The Sun may form a planetary nebula, but the outcome is uncertain.
Type I Supernovae have no hydrogen lines in the spectrum.
In many cases, the mass transfer cycle resumes after a nova explosion, leading to a cycle of repeating explosions every few years to decades.
Heavy-Element Fusion in high-mass stars (> 8 MSun), leading to the formation of an inert iron core, occurs in the final stages of fusion and ends extremely rapidly, converting 2 M⊙ of Si into Fe in just ~1 day.
Nova explosion.
Supernovae can be seen easily in distant galaxies.
Explosive onset of Hydrogen fusion.
If an accreting White Dwarf exceeds the Chandrasekhar mass limit, it collapses, triggering a Type I Supernova.
T Pyxidis is a recurrent nova.
Iron core ultimately collapses, triggering an explosion that destroys the star: A supernova.
The Sun’s Carbon and Oxygen core will become a White Dwarf.
The Remnant of SN 1987A is a ring, created by stellar wind, but made to glow brightly by the X-rays released during the first hour of the Supernova explosion.
Type I Supernovae are caused by the collapse of an accreting White Dwarf exceeding the Chandrasekhar mass limit.
Very hot, dense layer of non-fusing hydrogen on the White Dwarf surface.
The Sun will expand to a red giant approximately 5 billion years from now, expanding to the size of Earth’s orbit and incinerating Earth.
Accretion disk accumulates on the surface of the White Dwarf.
In the next decade, the expanding SN debris will reach the inner ring, causing the ring to brighten as it is obliterated by the collision.
SN 1987A was an unusual type II Supernova in the Large Magellanic Cloud in February 1987, one of only 7 SN in all of history that were bright enough to see without a telescope.
Eighteen hours before SN 1987A was first seen at optical wavelengths, detectors on Earth recorded 19 neutrinos arriving from the direction of the supernova, a burst that dramatically exceeded the background of low-energy sporadic neutrinos normally detected.
Type II Supernovae are caused by the explosive onset of Hydrogen fusion.