How Far Is It To The Center Of The Milky Way/Tootsie Pop?

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Discussion Overview

The discussion revolves around the challenges of measuring distances and sizes related to black hole singularities and the centers of galaxies. It touches on concepts from general relativity, including length contraction, the nature of singularities, and the implications of spacetime curvature.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that measuring distance to a black hole singularity is problematic due to length contraction and the undefined nature of such distances.
  • Others argue that instead of measuring distances, one can measure the area of spheres around the singularity, relating it to the radial coordinate through the formula ##A=4\pi r^2##.
  • A participant asserts that the "center" of a galaxy, referring to the singularity, is not a spatial point but a moment in time, which complicates measurements.
  • Some participants express that the distance from the singularity to other points is undefined, and thus traditional measurements like radius or diameter do not apply.
  • There is a discussion about the nature of singularities, with some stating they are not part of spacetime while others suggest they can be treated as boundaries within spacetime.
  • Participants debate the fate of objects falling into a singularity, with differing views on whether they are "frozen in time" or "destroyed" upon reaching the singularity.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of singularities, the feasibility of measuring distances in their vicinity, and the implications of objects interacting with them. The discussion remains unresolved with no consensus reached.

Contextual Notes

The discussion highlights limitations in current models of black holes and singularities, including the lack of a more realistic model to replace idealized representations. There are also unresolved assumptions regarding the definitions of distance and time in the context of singularities.

Daleri Mc Rileda
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With length contraction being ever increased while approaching the mass of a black hole singularity, how does one measure the distance to the virtual infinite contracting frames of reference of time and space /distance of the singularity? Related question : How can one measure the size of a galaxy passing through it's center /singularity?
 
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Please don't tag your threads with the "A" prefix unless you are prepared for an answer appropriate for a physics PhD candidate - in the relativity forum that would mean that you have studied and understand something at the level of http://www.staff.science.uu.nl/~hooft101/lectures/genrel_2010.pdf.

We have corrected the thread tag for you.
 
Daleri Mc Rileda said:
With length contraction being ever increased while approaching the mass of a black hole singularity, how does one measure the distance to the virtual infinite contracting frames of reference of time and space /distance of the singularity?
As you seemed to have intuitively understood, you cannot just lay a measuring rod to measure that distance. And because of the curvature of spacetime it would not mean the same thing anyway.

Instead, what is measured is the area of the sphere around the singularity. The unmeasurable radial coordinate is related to that measurable area by ##A=4\pi r^2##
 
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Daleri Mc Rileda said:
With length contraction being ever increased while approaching the mass of a black hole singularity

This is not correct.

Daleri Mc Rileda said:
the virtual infinite contracting frames of reference of time and space /distance

I don't know what you mean by this.

Daleri Mc Rileda said:
How can one measure the size of a galaxy passing through it's center

You can't, because the "center" of the galaxy (assuming that you mean the singularity at ##r = 0## of the black hole at the center of the galaxy) is not a point in space. It's a moment of time, which is to the future of anyone inside the hole's horizon.
 
Daleri Mc Rileda said:
how does one measure the distance to the virtual infinite contracting frames of reference of time and space /distance of the singularity? Related question : How can one measure the size of a galaxy passing through it's center /singularity?
The quick answer is that you don't - the "distance" from the central singularity to anywhere else is undefined, as is the "diameter" passing through the singularity.

The longer answer: although the distance to the singularity is undefined, and therefore there is no such thing as a radius or diameter, there is a quantity that we can use outside the event horizon. Consider two imaginary spheres centered on the black hole. The first one has surface area ##A_1=4\pi{r_1}^2## and the second has surface area ##A_2=4\pi{r_2}^2## - we can measure these surface areas and calculate ##r_1## and ##r_2## from them. These values ##r_1## and ##r_2## are not distances from the center, and the difference between them is not the distance between the surface of the smaller sphere and the larger sphere - but we can use them to label points around the black hole.

If you have a spherical galaxy with a black hole in the center, and someone says that it is ##X## lightyears across... They are really saying that the surface area of the galaxy is ##X\pi## square lightyears. If the black hole weren't there then the galaxy would be ##X## lightyears across... But it is there, so the distance across is undefined.
 
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Nugatory said:
The quick answer is that you don't - the "distance" from the central singularity to anywhere else is undefined, as is the "diameter" passing through the singularity.

The longer answer: although the distance to the singularity is undefined, and therefore there is no such thing as a radius or diameter, there is a quantity that we can use outside the event horizon. Consider two imaginary spheres centered on the black hole. The first one has surface area ##A_1=4\pi{r_1}^2## and the second has surface area ##A_2=4\pi{r_2}^2## - we can measure these surface areas and calculate ##r_1## and ##r_2## from them. These values ##r_1## and ##r_2## are not distances from the center, and the difference between them is not the distance between the surface of the smaller sphere and the larger sphere - but we can use them to label points around the black hole.

If you have a spherical galaxy with a black hole in the center, and someone says that it is ##X## lightyears across... They are really saying that the surface area of the galaxy is ##X\pi## square lightyears. If the black hole weren't there then the galaxy would be ##X## lightyears across... But it is there, so the distance across is undefined.
Thank you
 
Dale said:
As you seemed to have intuitively understood, you cannot just lay a measuring rod to measure that distance. And because of the curvature of spacetime it would not mean the same thing anyway.

Instead, what is measured is the area of the sphere around the singularity. The unmeasurable radial coordinate is related to that measurable area by ##A=4\pi r^2##
Thanks
 
PeterDonis said:
This is not correct.
I don't know what you mean by this.
You can't, because the "center" of the galaxy (assuming that you mean the singularity at ##r = 0## of the black hole at the center of the galaxy) is not a point in space. It's a moment of time, which is to the future of anyone inside the hole's horizon.
It should be no space and no time.
 
Daleri Mc Rileda said:
It should be no space and no time.

Do you mean the singularity? If so, your statement is incorrect. It would be correct to say that the singularity itself, strictly speaking, is not part of spacetime. But it can still be treated as a limit, a boundary of spacetime inside the horizon, and in that sense, it is a moment of time, not a place in space. (In more technical language, it is a spacelike line, not a timelike one.)
 
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PeterDonis said:
Do you mean the singularity? If so, your statement is incorrect. It would be correct to say that the singularity itself, strictly speaking, is not part of spacetime. But it can still be treated as a limit, a boundary of spacetime inside the horizon, and in that sense, it is a moment of time, not a place in space. (In more technical language, it is a spacelike line, not a timelike one.)
OK, I see what you are saying, frozen time.
 
  • #11
Daleri Mc Rileda said:
I see what you are saying, frozen time.

No, that's not what I was saying. Objects falling into the singularity are not "frozen in time". According to the idealized classical model we are discussing, they hit the singularity and are destroyed.
 
  • #12
PeterDonis said:
No, that's not what I was saying. Objects falling into the singularity are not "frozen in time". According to the idealized classical model we are discussing, they hit the singularity and are destroyed.
I don't understand what you mean by, "destroyed".
 
  • #13
Daleri Mc Rileda said:
I don't understand what you mean by, "destroyed".

It means that, according to this idealized model, objects that hit the singularity cease to exist. Bear in mind that this is an idealized model and physicists don't believe it's actually realistic. The problem is that we don't have a more realistic model to replace it with at this point.
 
  • #14
PeterDonis said:
It means that, according to this idealized model, objects that hit the singularity cease to exist. Bear in mind that this is an idealized model and physicists don't believe it's actually realistic. The problem is that we don't have a more realistic model to replace it with at this point.
OK
 

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