lpetrich
Contributor
As far as we can tell, the Universe is going to keep on expanding and running down, becoming thinner and thinner and colder and colder, making the "Big Freeze". Alternate possibilities are recollapse, the "Big Crunch", and superfast expansion, the "Big Rip".
The Five Ages of the Universe, Future of an expanding universe, [astro-ph/9701131] A Dying Universe: The Long Term Fate and Evolution of Astrophysical Objects
Our Universe has aged over a large spread of timescales, and it will continue to do so. Meaning that overall changes happen slower and slower as it ages. Oo it is convenient to use "cosmological decades" for its age at each point:
Age = 10^(dec)
Fred Adams and Gregory Laughlin in their book "The Five Ages of the Universe" divide up the Universe's history into these ages: Primordial, Stelliferous, Degenerate, Black-Hole, and Dark.
The Primordial Era (-50 < dec < 5): quantum gravity - cosmic inflation - freezeout of hadrons - freezeout of electrons and neutrinos - primordial nucleosynthesis - recombination of electrons and nuclei, making the Universe transparent to visible light
The Stelliferous Era (5 < dec < 14): what we are in now, decade 10. Stars form from interstellar dust and gas, then spew much of their substance back into it, often with relatively heavy elements formed by nucleosynthesis in their cores. It will end when there is too little interstellar material to form new stars.
Galaxies form early in this era (dec around 8 or 9), and gradually merge, forming giant elliptical galaxies. The Milky Way and the Andromeda Galaxy will eventually merge, forming a "Milkomeda" galaxy. That galaxy will eventually swallow up all the smaller Local-Group galaxies, like the Magellanic Clouds.
The Degenerate Era (14 < dec < 40): all the stars are burned out, leaving only white dwarfs, neutron stars, and black holes. The first two are composed of forms of degenerate matter, thus the name.
Around decades 15 - 16, planets are either ejected by other stars or else spiral into their stars by gravitational radiation.
G-rad: dec = 19.4 + 4*log10(a/AU) - 3*log10(M/Msun)
Eject: dec = 15.1 - 2*log10(a/AU)
Galaxies gradually evaporate as some of their stars acquire enough velocity to escape them from near-collisions. As they do so, the remaining stars get closer and closer together. Most stars may escape, with the remaining ones falling into the central black hole that most galaxies seem to have. If stars collide, then that may make a new star or even a supernova.
If otherwise-stable nucleons can decay, then at around 100 times their half-life, all the white dwarfs, neutron stars, and other baryonic-matter bodies will all be gone. For a half-life a little above experimental limits, about dec = 36, that disappearance time becomes dec = 38. This is for single-nucleon decay, and nucleons may instead decay in two-nucleon or three-nucleon processes, or even processes involving virtual black holes. However, these processes are expected to be much slower than single-nucleon processes, with half-lives up to dec = 200 or more.
These objects don't disappear right away, of course, but very slowly. Above about Jupiter mass, they slowly expand until they become Jupiter-sized, and then they slowly shrink. Neutron stars have an ordinary-matter crust, and as nucleons decay, that crust expands and the neutronium part shrinks until at about 0.09 solar masses, the neutronium disappears and the star is much like a white dwarf.
The Black-Hole Era (40 < dec < 100): If nucleons have decayed, all that will be left will be black holes. They will glow by the Hawking mechanism, giving them a lifetime of
dec = 65 + 3*log10(M/Msun)
While a solar-mass black hole will decay in dec = 65, a galaxy-mass black hole (10^11 solar masses) will decay in dec = 98.
The Dark Era (100 < dec): all that is left is very-low-density and very-low-energy photons, electrons, and positrons.
What happens next is very speculative. The simplest fate is to continue to expand forever, but other things might happen.
The Five Ages of the Universe, Future of an expanding universe, [astro-ph/9701131] A Dying Universe: The Long Term Fate and Evolution of Astrophysical Objects
Our Universe has aged over a large spread of timescales, and it will continue to do so. Meaning that overall changes happen slower and slower as it ages. Oo it is convenient to use "cosmological decades" for its age at each point:
Age = 10^(dec)
Fred Adams and Gregory Laughlin in their book "The Five Ages of the Universe" divide up the Universe's history into these ages: Primordial, Stelliferous, Degenerate, Black-Hole, and Dark.
The Primordial Era (-50 < dec < 5): quantum gravity - cosmic inflation - freezeout of hadrons - freezeout of electrons and neutrinos - primordial nucleosynthesis - recombination of electrons and nuclei, making the Universe transparent to visible light
The Stelliferous Era (5 < dec < 14): what we are in now, decade 10. Stars form from interstellar dust and gas, then spew much of their substance back into it, often with relatively heavy elements formed by nucleosynthesis in their cores. It will end when there is too little interstellar material to form new stars.
Galaxies form early in this era (dec around 8 or 9), and gradually merge, forming giant elliptical galaxies. The Milky Way and the Andromeda Galaxy will eventually merge, forming a "Milkomeda" galaxy. That galaxy will eventually swallow up all the smaller Local-Group galaxies, like the Magellanic Clouds.
The Degenerate Era (14 < dec < 40): all the stars are burned out, leaving only white dwarfs, neutron stars, and black holes. The first two are composed of forms of degenerate matter, thus the name.
Around decades 15 - 16, planets are either ejected by other stars or else spiral into their stars by gravitational radiation.
G-rad: dec = 19.4 + 4*log10(a/AU) - 3*log10(M/Msun)
Eject: dec = 15.1 - 2*log10(a/AU)
Galaxies gradually evaporate as some of their stars acquire enough velocity to escape them from near-collisions. As they do so, the remaining stars get closer and closer together. Most stars may escape, with the remaining ones falling into the central black hole that most galaxies seem to have. If stars collide, then that may make a new star or even a supernova.
If otherwise-stable nucleons can decay, then at around 100 times their half-life, all the white dwarfs, neutron stars, and other baryonic-matter bodies will all be gone. For a half-life a little above experimental limits, about dec = 36, that disappearance time becomes dec = 38. This is for single-nucleon decay, and nucleons may instead decay in two-nucleon or three-nucleon processes, or even processes involving virtual black holes. However, these processes are expected to be much slower than single-nucleon processes, with half-lives up to dec = 200 or more.
These objects don't disappear right away, of course, but very slowly. Above about Jupiter mass, they slowly expand until they become Jupiter-sized, and then they slowly shrink. Neutron stars have an ordinary-matter crust, and as nucleons decay, that crust expands and the neutronium part shrinks until at about 0.09 solar masses, the neutronium disappears and the star is much like a white dwarf.
The Black-Hole Era (40 < dec < 100): If nucleons have decayed, all that will be left will be black holes. They will glow by the Hawking mechanism, giving them a lifetime of
dec = 65 + 3*log10(M/Msun)
While a solar-mass black hole will decay in dec = 65, a galaxy-mass black hole (10^11 solar masses) will decay in dec = 98.
The Dark Era (100 < dec): all that is left is very-low-density and very-low-energy photons, electrons, and positrons.
What happens next is very speculative. The simplest fate is to continue to expand forever, but other things might happen.