Shapes of black holes (energy talk)

In summary: The surface of the black hole is simply the limit of all the solutions that approach it from outside.
  • #1
1832vin
58
1
ok, hear me out on a lymph, because I'm going to either be talking crap or something that sounds crazy
either way...
my question is:
why does the phenomena of a black hole look so perfectly circular/spherical?
now here's my reasoning

spheres are the shape that takes the least energy to be sustained due to the ration of squares numbers and cube numbers

now if you start heating a bubble which had little energy, then the surface starts to wobble, and then it bursts, because objectively speaking, more energy makes things go out of the state the least energy, from electron shells to bubbles,

p.s., i know the sun is quite spherical to look at from far, far away, but the energy density of it is still nothing compared to a black hole which is suspected to interfere with time due to it amount in energy

but then why is that, a black hole which is said to have the highest energy density, appear to be so perfectly circular (ie, there is suppose to be a disk of gravity limit) it may be because we are very far, but still too perfectly circular in my perspective...

what do you think about my ridiculous thought?
 
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  • #2
A black hole is actually a point (or so we think. It's a singularity - which means we don't really know what it is). When we talk about the shape of a black hole, we are usually talking about the event horizon. The event horizon is not a physical object; it is simply the boundary beyond which light cannot escape.

Naturally, the boundary will be equidistant from the central point in all directions.

Make sense?

P.S. What this mean?
... hear me out on a lymph ...
 
  • #3
DaveC426913 said:
A black hole is actually a point (or so we think. It's a singularity - which means we don't really know what it is). When we talk about the shape of a black hole, we are usually talking about the event horizon. The event horizon is not a physical object; it is simply the boundary beyond which light cannot escape.

Naturally, the boundary will be equidistant from the central point in all directions.

Make sense?

P.S. What this mean?

hear me out on a lymph ... = don't take it too seriously

but yeah, why is it equidistant? i get that when you draw a shape with constant distance from center point, you'd get a circle

but normal (objectly speaking) the higher the energy, the further away from pi it'd tend to be, so it's wouldn't it be either : event horizon is not really circular, or, there is a even bigger counter force that makes it low enough energy to have a good relationship with pi
 
  • #4
1832vin said:
hear me out on a lymph ... = don't take it too seriously
Lymph is a bodily fluid...o_O

1832vin said:
but yeah, why is it equidistant? i get that when you draw a shape with constant distance from center point, you'd get a circle
A circle is two dimensional. In 3 dimensional space, you'd get a sphere.

1832vin said:
but normal (objectly speaking) the higher the energy, the further away from pi it'd tend to be,
Why?

1832vin said:
event horizon is not really circular,
No, it's spherical.

1832vin said:
or, there is a even bigger counter force that makes it low enough energy to have a good relationship with pi
What?
 
  • #5
Only Schwarzschild BH is spherically symmetric. More complicated BHs aren't.
 
  • #6
1832vin said:
why does the phenomena of a black hole look so perfectly circular/spherical?

The first step in the derivation of the Schwarzschild solution to the Einstein Field Equations is "assume that the gravitating body is spherical". It is, therefore, somewhat less than surprising that the resulting solution describes a spherically symmetric black hole.

It doesn't follow from this that an actual physical black hole is a perfect sphere - it's not!. The spherical solution is a very good approximation so we use it, just as we treat the Earth as a sphere instead of the slightly lumpy and pear-like shape that it actually is, when calculating orbits.
 
  • #7
To add to the above, equidistant is a misnomer here. The r coordinate is time-like inside the horizon and there is no "distance" to the singularity in that sense. There is also nothing strange about the spherical symmetry - it only holds for black holes without angular momentum. Black holes with angular momentum do not exhibit spherical symmetry.
 
  • #8
Orodruin said:
Black holes with angular momentum do not exhibit spherical symmetry.

Even if they have a spherically symmetric density? So spherical fronts comprising the black hole, and the density at any point on this shell is uniform in density. I'm having trouble picturing how that would come out.
 
  • #9
BiGyElLoWhAt said:
Even if they have a spherically symmetric density? So spherical fronts comprising the black hole, and the density at any point on this shell is uniform in density. I'm having trouble picturing how that would come out.

Solutions like the Schwarzschild solution are vacuum solutions, there is no mass density distribution.
 
  • #10
If there is no density, then how can it have angular momentum about its center of mass?
 
  • #11
There are some different ways of defining mass in GR. You should not be surprised to find the Schwarzschild solution a vacuum solution. After all, it describes the solution outside of a spherically symmetric distribution. (There is also an internal solution, but that is not what I am discussing)
 
  • #12
Yes, but I don't see how rotation affects the symmetry. Does it not still have the spatial symmetry? I understand that there is 0 matter distributed outside the horizon, but the symmetry of spacetime outside should be dependant on the symmetry of matter within. Conceptually speaking, of course, I have never even attempted to derive a solution to EFE.
 
  • #13
Indeed the Schwarchzild black hole is a vacuum solution, because the energy-momentum tensor is zero everywhere in your spacetime (except for the r=0 point, where you have the singularity, but oh well that's outside the spacetime). Choosing appropriate coordinates (coordinate invariance of EFEs allow it) you can take that there is no density either.
A Schwarchzild black hole is not rotating.

Then why rotating objects break the spherical symmetry? That's even known from Newtonian mechanics, and a great example of it is the non-spherical shape of the Earth (due to its rotation). In particular in classical mechanics, instead of just the gravitational potential, you will also get some potential due to the rotation, which will change the spherically symmetric solutions.
 
  • #14
BiGyElLoWhAt said:
Yes, but I don't see how rotation affects the symmetry. Does it not still have the spatial symmetry? I understand that there is 0 matter distributed outside the horizon, but the symmetry of spacetime outside should be dependant on the symmetry of matter within. Conceptually speaking, of course, I have never even attempted to derive a solution to EFE.
Rotation breaks the full rotational symmetry by introducing a preferred direction, the axis of rotation. You should not expect the solution to be spherically symmetric (and indeed it is not, see http://en.wikipedia.org/wiki/Kerr_metric).
 
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  • #15
BiGyElLoWhAt said:
Yes, but I don't see how rotation affects the symmetry. Does it not still have the spatial symmetry? I understand that there is 0 matter distributed outside the horizon, but the symmetry of spacetime outside should be dependant on the symmetry of matter within. Conceptually speaking, of course, I have never even attempted to derive a solution to EFE.

The Einstein field equations include not just the distribution of matter but also the distribution of stress and energy. Even if you have a spherically symmetric matter distribution, it is clear that if your spherically symmetric mass is rotating the distribution of stress and energy is not going to be spherically symmetric (it will be different at the poles and the equator) so the spacetime that solves the EFE will also not be spherically symmetric.

And that's before your initially spherically symmetric mass distribution starts moving around because it's not in a spherically symmetric spacetime...
 
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  • #16
Yes, yes, I overlooked that. Thanks for pointing that out to me, guys.
 

Related to Shapes of black holes (energy talk)

1. What is a black hole?

A black hole is a region in space with a gravitational pull so strong that nothing, including light, can escape from it. This is due to the immense amount of matter packed into a small space, creating a strong gravitational field.

2. How do black holes form?

Black holes are formed when a massive star dies and collapses under its own gravity. This can also happen when two or more smaller black holes merge together.

3. What is the shape of a black hole?

The shape of a black hole is determined by its spin and the amount of matter it contains. The most commonly accepted shape is a spherical event horizon, also known as the Schwarzschild radius.

4. Can black holes have different shapes?

Yes, black holes can have different shapes depending on their spin and the effects of nearby matter. They can also have an oblate or prolate shape if they are spinning rapidly.

5. How do scientists study the shapes of black holes?

Scientists use various techniques to study the shapes of black holes, including observing their effects on nearby matter and using mathematical models and simulations. They also use telescopes and other instruments to study the radiation emitted from the event horizon of a black hole.

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