Question about Schwarzschild radius

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Discussion Overview

The discussion revolves around the concept of Schwarzschild radius, particularly in relation to black holes and gravitational singularities. Participants explore theoretical implications, analogies, and the conditions under which an object can be considered a black hole, as well as the gravitational effects involved.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that if an object is compressed to its Schwarzschild radius, it will collapse into a black hole, using the sun as an example.
  • Others argue that while the gravitational pull of an object remains constant, the effective gravity experienced by light changes as the object is compressed, potentially trapping light within the Schwarzschild radius.
  • A participant presents a calculation of their own Schwarzschild radius, questioning whether compression would prevent light from escaping.
  • Some participants suggest that every object has a Schwarzschild radius, but others clarify that the mass within that radius must be considered, and not all objects can be treated as black holes.
  • There is a discussion about the validity of Schwarzschild radius calculations within the context of objects like the sun, with some asserting that the assumptions of the calculations do not hold in such cases.
  • One participant mentions that the concept of Schwarzschild radius is useful when discussing the conditions under which an object could become a black hole, particularly when compressed below that radius.
  • Another participant notes that even small objects, like a golf ball, technically have a Schwarzschild radius, albeit very small.
  • Concerns are raised about the gravitational pull of the sun remaining constant, leading to confusion about how it could ever become a black hole.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the implications of Schwarzschild radius and the conditions necessary for an object to be considered a black hole. The discussion remains unresolved, with differing interpretations of gravitational effects and the significance of Schwarzschild radius in various contexts.

Contextual Notes

Limitations include the dependence on assumptions about mass distribution and the conditions under which Schwarzschild radius calculations are valid. The discussion highlights the complexities involved in applying these concepts to real-world objects like the sun.

zeromodz
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Okay, correct me if I am wrong but Schwarzschild radius of an object if it squeezed to a radius of that point it will collapse into a gravitational singularity and become a black hole. For example, if the sun has a Schwarzschild radius of about 3 kilometers. If we were to be squeezed the sun to that diameter, it would theoretically collapse into a black hole right?

If that is true, I don't understand. Even if you squeeze the sun into a gravitational singularity, it would still have the same gravity, which is not efficient enough to trap light. So how can this be true?
 
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Roughly, everything will look the same if you stay outside the Schwarzschild radius, but once you go past the Schwarzschild radius, you are doomed. In fact, part of the Schwarzschild solution is appropriate for the region of space outside the sun, even now when it is not a black hole.
 
zeromodz said:
If that is true, I don't understand. Even if you squeeze the sun into a gravitational singularity, it would still have the same gravity, which is not efficient enough to trap light. So how can this be true?

It would have greater gravity. The center of gravity of the sun is a long way away from a grazing light beam. At a much smaller diameter the grazing light beam would be much closer to the center of mass.
 
Phrak said:
It would have greater gravity. The center of gravity of the sun is a long way away from a grazing light beam. At a much smaller diameter the grazing light beam would be much closer to the center of mass.


So your saying that, for instance I take my own Schwarzschild radius which would be
(2)(M)(G)/(C^2)
(2)((145*1.45)/9.8)(6.674 * 10^-11)/(299972458^2)
= 3.18628575 * 10^-26 meters

If I were compressed into a sphere, not even light could escape me if it traveled that close to the center of my mass?
 
If you want to think about this in a Newtonian analogy, you can do so as follows (note, in Newtonian gravity, light is not bent by gravity, but I think there is still some worth to the analogy):
While the sun is as large as it is, a body can only come so close before contacting the sun's surface. Therefore the maximum field produced by the sun is,
[tex]g_{max}=\frac{G M_{sol}}{r_{sol}^2}[/tex]
As we compress the sun, the max field increases until at some point this field is so strong not even light escapes, and we have reached the Schwarzschild radius for compression.

It is just an analogy, but I think it helps to demonstrate why gravity seems "stronger".
 
zeromodz said:
So your saying that, for instance I take my own Schwarzschild radius which would be
(2)(M)(G)/(C^2)
(2)((145*1.45)/9.8)(6.674 * 10^-11)/(299972458^2)
= 3.18628575 * 10^-26 meters

If I were compressed into a sphere, not even light could escape me if it traveled that close to the center of my mass?

That's the theory, yes.
 
Nabeshin said:
(note, in Newtonian gravity, light is not bent by gravity, but I think there is still some worth to the analogy)

It is, if light is assumed to have an equivalent mass due to energy--but this is a side issue.
 
Phrak said:
That's the theory, yes.

So one more verification. Does this mean that every object possesses a black hole, its just the objects we call black holes have a Shcwarzchild's radius that is extremely large compared to other objects? So the center of the sun from 3 kilometers away is completely black and a black hole itself?
 
zeromodz said:
So one more verification. Does this mean that every object possesses a black hole, its just the objects we call black holes have a Shcwarzchild's radius that is extremely large compared to other objects? So the center of the sun from 3 kilometers away is completely black and a black hole itself?

No, not at all. Consider that within a radius of 3km around the sun is only so much mass (I'd do a calculation but I'm lazy). The point is, it is much less than the mass of the entire sun. It is only the enclosed mass that you have to trouble yourself with, so you would see that the schwarzschild radius for this amount of mass would be some much smaller number, 1m or something. But you run into the same problem if you try and say "so there's a black hole at r=1m right?"

Does this make sense?
 
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  • #10
Nabeshin said:
No, not at all. Consider that within a radius of 3km around the sun is only so much mass (I'd do a calculation but I'm lazy). The point is, it is much less than the mass of the entire sun. It is only the enclosed mass that you have to trouble yourself with, so you would see that the schwarzschild radius for this amount of mass would be some much smaller number, 1m or something. But you run into the same problem if you try and say "so there's a black hole at r=1m right?"

Does this make sense?

Well, wouldn't that put you into an infinite regression? I don't understand
 
  • #11
Yes, it would. And it serves to show there is no black hole located anywhere inside the sun!

The calculation of schwarzschild radius assumes that the entire mass of the object is concentrated at a point, ok? That's all well and good, but you can only assume this when you're talking about the area outside of the object (in this case, outside the sun). So when you get a schwarzschild radius inside the sun, you recognize that your results are no longer valid because the assumptions were not met in the first place.
 
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  • #12
Nabeshin said:
Yes, it would. And it serves to show there is no black hole located anywhere inside the sun!

The calculation of schwarzschild radius assumes that the entire mass of the object is concentrated at a point, ok? That's all well and good, but you can only assume this when you're talking about the area outside of the object (in this case, outside the sun). So when you get a schwarzschild radius inside the sun, you recognize that your results are no longer valid because the assumptions were not met in the first place.

So, then what is the point of schwarzschilds radius? What do physicsist use it for? Does that mean no object unless the entire mass of an object is concentrated at a point like a singularity of a black hole has a schwarzschilds radius? Does this mean the Schwarszchilds radius for any other object besides black holes are invalid?
 
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  • #13
Sort of. It can be a useful concept (this might sound recursive but I think if you read the post I gave above it'll make more sense) when the object is fully contained within the schwarzschild radius. Although this doesn't a priori mean that it has to be a black hole, it does mean that it eventually does have to become one.

And yes, it's sort of silly to talk about the schwarzschild radius of the sun or the Earth or anything like that, because it has no physical significance (i.e there's nothing special if you went to 3km from the center of the sun). Usually people use it by saying "if you compressed the sun to a 3km sphere, you would form a black hole" which is where you can make the concept useful. It only becomes meaningful when the object is compressed to less than that radius.
 
  • #14
Technically, a golf ball has a Schwartzchild Radius. The radius is of course very small, but it's a real, physical radius nonetheless.
 
  • #15
Nabeshin said:
Usually people use it by saying "if you compressed the sun to a 3km sphere, you would form a black hole" which is where you can make the concept useful. It only becomes meaningful when the object is compressed to less than that radius.
But that brings me back to my first problem. The sun always has the same gravitational pull though, how can it ever turn into a black hole? It doesn't matter how much you compress it, even if the radius falls below Schwarzschilds radius. It will always have the same pull, am I wrong?
 
  • #16
Refer to my post #5... Umm, I don't know how else to explain it other than how I have so I'll let someone else give it a try and hopefully succeed better.
 
  • #17
Nabeshin said:
Refer to my post #5... Umm, I don't know how else to explain it other than how I have so I'll let someone else give it a try and hopefully succeed better.

Alright man, thanks for helping:)
 
  • #18
zeromodz said:
But that brings me back to my first problem. The sun always has the same gravitational pull though, how can it ever turn into a black hole? It doesn't matter how much you compress it, even if the radius falls below Schwarzschilds radius. It will always have the same pull, am I wrong?

As you already know, all objects fall at the same rate on the moon because the moon doesn't have an atmosphere to slow things down. Now to answer your question:

Suppose you're on the moon, and you have two objects of equal mass: The first object is a lead pellet, and the other object is a huge ball of aerogel that's 1 foot in diameter. Remember, they both weigh the same and are of equal mass.
Now drop both objects onto a very thin sheet of cellophane that's suspended 1 foot from the lunar surface. Which object caused the most stretching of the sheet of cellophane? That's right: the lead pellet. They are both of equal mass, yet the pellet did more damage! How can that be? They're of equal mass, after all!

Likewise, consider two interstellar objects: the first object is the Sun, and the second object is exactly as massive as the Sun, only it had been compressed to a diameter of only 3Km. Which interstellar object will have the greater gravitational pull at its surface (important)? The Sun? Or the 3Km object? That's right: Since the Sun has its gravitational field distributed and weakened over a very, very large area equal to its very large radius (minus 3 Km), and the 3Km object has its gravitational pull concentrated and strengthened to a very fine point, the 3Km object will by far exert the greater gravitational pull at its surface (again, important!) even though both objects are of equal mass.
 
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  • #19
Neo_Anderson said:
Technically, a golf ball has a Schwartzchild Radius. The radius is of course very small, but it's a real, physical radius nonetheless.

From what I have casually read on the subject, Neo_Anderson is technically correct. However, I believe a golf ball's S-Radius (which I assume is EXTREMELY tiny) will display none of the effects that one would typically associate with an S-Radius unless all of the mass of that object (the golf ball, in this case) were to be completely compacted within that S-Radius. And since that never happens to most golf balls I know, the S-Radius of a golf ball has no practical meaning, does it?

Daisey
 
  • #20
daisey said:
From what I have casually read on the subject, Neo_Anderson is technically correct. However, I believe a golf ball's S-Radius (which I assume is EXTREMELY tiny) will display none of the effects that one would typically associate with an S-Radius unless all of the mass of that object (the golf ball, in this case) were to be completely compacted within that S-Radius. And since that never happens to most golf balls I know, the S-Radius of a golf ball has no practical meaning, does it?

Daisey

The schwartzchild's golfball would evaporate in like 0.00002 nanoseconds.
 
  • #21
daisey said:
From what I have casually read on the subject, Neo_Anderson is technically correct. However, I believe a golf ball's S-Radius (which I assume is EXTREMELY tiny) will display none of the effects that one would typically associate with an S-Radius unless all of the mass of that object (the golf ball, in this case) were to be completely compacted within that S-Radius. And since that never happens to most golf balls I know, the S-Radius of a golf ball has no practical meaning, does it?

Daisey
I wouldn't associate any effects with a Schwarzschild radius specifically. The effects (extreme gravity etc.) are associated with a black hole, which would only exist if the golf ball were to be compressed down to some particular size.
 
  • #22
zeromodz said:
But that brings me back to my first problem. The sun always has the same gravitational pull though, how can it ever turn into a black hole? It doesn't matter how much you compress it, even if the radius falls below Schwarzschilds radius. It will always have the same pull, am I wrong?
The Sun always has the same gravitational pull at a given radius outside of the Sun. If you compare the Sun's gravitational pull at two different radii, they will be different. If you compare the Sun's gravitational pull at the same radius in two different situations, if that radius lies within the Sun in either of the situations, they will be different. Saying "the Sun always has the same gravitational pull" only applies if you compare it at the same radius outside the Sun.

If you shrink the Sun down to its Schwarzschild radius, then at the Earth's orbit, the gravitational pull will be the same because the Earth is outside of the Sun whether it's a black hole or not. (Contrast: if the Sun were to expand into a red giant, so that it actually became larger than the Earth's orbital radius, that would change its gravitational pull on the Earth.)

Another way to think about it is that the Sun has a certain "Schwarzschild density." If you were to compress the Sun, or any solar-mass object, to that density, it would become a black hole. As long as it is less dense than that, it is not a black hole.
 
  • #23
zeromodz said:
But that brings me back to my first problem. The sun always has the same gravitational pull though, how can it ever turn into a black hole? It doesn't matter how much you compress it, even if the radius falls below Schwarzschilds radius. It will always have the same pull, am I wrong?

No, it does not always have the same pull. Mercury experiences a much greater gravitational pull from the sun than planet Earth, because gravitational pull increases as you get closer to the sun. However, you can only get so close before you actually run into the sun.

If the sun was smaller (with same mass), then you could effectively get closer to it, and so you would experience an even greater gravitational pull.

The force of gravity is F=G*(M1M2)/r^2

That r^2 limits how much gravity an object can produce. If you can decrease it, gravity will increase. If you can decrease the sun's to 1.5km...well, you know the rest.

Another way to look at it is the warping of space time. Or, imagine laying down on a trampoline and warping it. If you stand up, your mass will be the same, but the warping right under your feet will be greater. If you have small feet, the trampoline will warp even more. If you attach a knife to each foot, your mass will still be the same, but your "radius" will be so small and the warping so great, that you will end up ripping right through the trampoline...kind of like how a black hole rips through space time.
 

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