The Gravo-Thermal Catastrophe

64 pointsposted 16 hours ago
by terryf

20 Comments

jessriedel

5 hours ago

Is this right?:

* Although you can make the enveloping sphere as large as you want, the (anti-)equilibration process requires a sphere of some finite radius because if you wait long enough a few stars eventually get launched at escape velocity, and if these actually escaped they would effectively cool the remaining stars.

* Therefore, the characteristic time scale for this process (i.e., the timescale on which the average kinetic energy rises substantially) gets longer and longer as the sphere gets larger.

* In order for the pressure and average speed of the stars to keep rising, the gravitational potential needs to keep falling, so at least some stars need to get and stay very close. In real life, these turn into black holes, which cuts off the process by limiting the amount of gravitational potential energy that can be unlocked in any given volume with a given mass.

pavel_lishin

5 hours ago

> In real life, these turn into black holes

I think this is right, and I think he explicitly calls out that these calculations were done with Newtonian physics modeling point particles - and we know that those two factors severely limit the application of this to the real-world.

jessriedel

3 hours ago

Right, it wasn't criticism, but the point I added (that I think was not explicit in the article) is this: black holes provide a lower bound on the potential energy, not just an indication that the model is breaking down.

pfdietz

4 hours ago

As I understand it, those simulations did not include three-body interactions that could leave particle pairs bound. If this happens, those binaries can now inject energy into the cluster as a whole, keeping it inflated and preventing collapse. Of course, the binaries' orbits shrink over time, so this doesn't go on forever.

leephillips

2 hours ago

What is a three-body interaction in classical gravity? If you calculate the force on each particle from every other particle, what’s left out?

AnotherGoodName

5 hours ago

My favourite along these lines is that the mass vs diameter relation for black holes scales in such a way that we are absolutely in a black hole right now according to current theory. As in the current mass of the universe is enough for a black hole with an event horizon diameter that extends beyond the universe.

Nesco

5 hours ago

This mass to event horizon radius relationship is a property of a Schwarzschild spacetime geometry, globally the universe has a FLRW spacetime geometry

trhway

25 minutes ago

The light has no chances of getting out of the 13.7B ly bubble due to Hubble expansion. Sounds a lot like black hole.

Nesco

12 minutes ago

The universe has no center, a black hole has one. The limits of the visible universe is an horizon on your frame of reference

In nerdspeak, the geometries are not the same, one is isotropic the other anisotropic

keskival

6 hours ago

I suppose in the real world such stars would collide in the center of the sphere and possibly form a black hole before achieving the required density approaching infinity, and also catapult stars out so that they leave the system by exceeding the escape velocity without encountering an elastic wall returning them to the system.

pdonis

5 hours ago

> in the real world such stars would collide in the center of the sphere and possibly form a black hole

Yes, the article mentions that towards the end.

trhway

4 hours ago

Application of the 1/R2 gravity formula to the pointwise mass with R->0 can easily power your Romulan ships. In similar vein applying that classical gravity formula - which is valid only to spherical masses or masses at such large distances that they can be treated as such - to the stars inside disk galaxies gets you the "dark matter", and thus not surprisingly the flatter the disk galaxy the more "dark matter" :)

meindnoch

3 hours ago

>In similar vein applying that classical gravity formula - which is valid only to spherical masses

What? Newtonian gravity is defined for point masses. Anything else you derive from that by integrating a mass density over a region.

trhway

3 hours ago

it is equivalent formulations - the point masses case is obtained from the spherical in the limit. The spherical case is just more illustrative to show where the fantom of the "dark matter" in the disk galaxies comes from.

>by integrating a mass density over a region.

exactly. When you do that for a disk galaxy you get much flatter curves that the 1/R the proponents of the dark matter insist on (that 1/R is exactly what one would get if the galaxy was spherical or the star was far outside of the disk)

bbor

3 hours ago

A) …why? What makes this interesting to physicists? I understand this as “if stars weren’t stars but instead rigid spheres, and if they were in an impossibly-impervious giant sphere, then weird stuff happens”. And…?

B) “since stars rather rarely collide” still blows my mind. I did some napkin math on Reddit a while back on why there will be very few stellar collisions (really, one star falling into another’s orbit?) when andromeda collides with the Milky Way, and the answer is that space is just mind-bogglingly huge. Even the most dense clusters in our galaxy are akin to ~70 1cm diameter spheres per olympic swimming pool.

If god is real, he is surely a giant.

LegionMammal978

2 hours ago

For A), if you have a bunch of tiny atoms bouncing around within a regular-sized sphere, then thermodynamics predicts that the sphere will experience some constant amount of pressure, with tiny fluctuations up and down. This result is interesting, since it just takes the ordinary system and asks, "What if we scale it up so that the atoms (stars) interact gravitationally?" Then, there is no equilibrium pressure experienced by the sphere, since the gravitational potential of the stars keeps increasing.

trhway

2 hours ago

> Then, there is no equilibrium pressure experienced by the sphere, since the gravitational potential of the stars keeps increasing.

And GR fixes that by kind of moving the sphere walls farther away, ie. the space geometry changing by the changing gravitational potential.

phkahler

7 hours ago

>> Also suppose they’re ‘gravitationally bound’. This means their total energy, kinetic and potential, is negative. That means they couldn’t all shoot off to infinity even if the sphere wasn’t there holding them in.

This seems like an invalid assumption. We know that clusters of stars can eject some of their members. Lot of hand waving in this one.

pavel_lishin

7 hours ago

That sentence does say "couldn't all shoot off to infinity".

ISL

7 hours ago

That's only an initial condition -- that requirement states only that the total energy is negative.

We are gravitationally bound to Earth, but the Voyagers have left the solar system.