Does Time Slow Down Near a Black Hole?

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Discussion Overview

The discussion revolves around the concept of time dilation near a black hole, specifically whether time slows down or stands still as one approaches a black hole. Participants explore various scenarios, including the experience of astronauts near a black hole, the effects of gravitational forces, and the implications of being observed from a distance.

Discussion Character

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

Main Points Raised

  • Some participants suggest that time appears to pass more slowly for an observer falling toward a black hole as seen by a distant observer, due to the effects of gravitational time dilation.
  • Others argue that while light escaping from near a black hole is redshifted and takes longer to reach distant observers, this does not imply that time itself is "slowing down" in a conventional sense.
  • A participant points out that one does not need to cross the event horizon to experience time dilation; even orbiting a black hole can result in significant differences in experienced time compared to an observer far away.
  • There is a discussion about the conditions under which significant time dilation occurs, particularly in relation to the photon sphere and the necessity of maintaining a powered orbit to avoid being drawn into the black hole.
  • Some participants express confusion about the terminology of "time slowing down," suggesting that it is a misconception and that time dilation should be understood in terms of spacetime curvature and the relative motion of observers.
  • Questions are raised about the extent of time dilation, with participants inquiring how much time could pass in the universe compared to the time experienced by someone close to a black hole.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the interpretation of time dilation near black holes, with multiple competing views and ongoing debate about the implications of gravitational effects and the nature of time itself.

Contextual Notes

Some limitations include the dependence on definitions of time and distance in the context of general relativity, as well as the complexity of the scenarios discussed, which may not be fully resolved within the conversation.

  • #31
C'mon, this is supposed to be the best theoretical physics forum on the entire internet. "Google relativistic calculator"

Let's work out the case of the photon rocket. Suppose in some frame the rocket is initially at rest in space. The four momentum is P1 = (M1,0). Then it burns anti-matter fuel and it's four momentum becomes P2= (M2 gamma, M2 gamma v). Conservation of four momentum:

P1 = P2 + Pf

where Pf is the total four momentum of the emitted photons and is thus of the form (E, -E). This means that:

Pf = P1 - P2

Square both sides and use that

Pf^2 = 0,

P1^2 = M1^2

P2^2 = M2^2

P1 dot P2 = gamma M1*M2

So we have:

0 = M1^2 + M2^2 - 2 gamma M1 M2 ----->

gamma = 1/2 [X + X^(-1)]

where X is the ratio of the final and initial mass

Note that if we use massive particles instead of photons Pf^2 would be strictly larger than zero and you would get a smaller gamma factor for the same initial/final mass ratio. So, the photon rocket is the best we can get.

Now, if we want to return to Earth we must put X= (M1/M2)^(1/4), where M1 is the initial mass of the rocket (which includes the fuel) and M2 the final mass. This is because we must accelerate to the gamma factor, and then change the direction of the velocity, which is equivalent to changing the velocity to zero and then back to the sama gamma factor but with the velocity in the opposite direction.

Then, when we reach Earth we must reduce the velocity to zero. If we want to travel at the same gamma factor during the trip, then the mass ratio's before and after the boosts must be the same each time, so X^4 = M1/M2


Now, we can play the following game. Suppose we have an anti-matter factory that produces anti-matter at a constant rate. We want to travel to some far away place, so we need a lot of antimatter. But, unfortunately, that takes a long time. An obvious strategy is to use some of the produced anti-matter to make small excursions. When we return form an excursion more time has passed in the frame of the factory, so we have a lot of anti-matter. If we do this right, we have more anti-matter than we would have had, had we stayed home despite using some for the excursion.

Now, if I remember correctly, it turns out that you can reduce the proper time you need to wait before you have the desired amnount of anti-matter be a factor of order Log(T/t), where T is the time needed to produce the anti-matter in the rest frame of the factory and t is the time needed to produce an amount of anti-matter equal to the mass of the rocket.
 
Last edited:
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  • #32
Chris Hillman said:
I forgot to mention that the bottomless fuel supply is an extremely dubious aspect regarding any proposal to accelerate a spaceprobe to near the speed of light using a conventional rocket engine.

No, but planetary lasers are the next best thing.
 
  • #33
Count Iblis said:
C'mon, this is supposed to be the best theoretical physics forum on the entire internet. "Google relativistic calculator"
You think the OP would rather have a half screen of calculation that leads to a single answer than be shown a tool where he can play to his heart's content?
 
  • #34
DaveC426913 said:
You think the OP would rather have a half screen of calculation that leads to a single answer than be shown a tool where he can play to his heart's content?


The relativistic calculators only give the formulae for the gamma factor as a function of velocity. Trivial stuff. And without knowledge of relativity you wouldn't be able to see that the gamma factor is simply 1/2 [X + X^(-1)] where X is the mass ratio before and after the burning of the anti-matter fuel. So, a 10^6 kg spacecraft carrying 10^6 kg antimatter fuel can reach a gamma factor of
(1/2)(2 + 1/2) = 1.25. And note that this formula was derived above in 13 (small) lines. The derivation was so simple that you can imagine doing it in your head without paper and pencil.

So, who needs the "relativistic calculator" :smile:
 
  • #35
I heard a theory that black holes exist on Earth, like really really tiny ones I read something about it being someone's theory when I read something about people contemplating making really really tiny black holes in a collider
um does anyone know about the theory about really small black holes already existing on Earth?
 
  • #36
bioquest said:
I heard a theory that black holes exist on Earth, like really really tiny ones I read something about it being someone's theory when I read something about people contemplating making really really tiny black holes in a collider
um does anyone know about the theory about really small black holes already existing on Earth?

That "theory" isn't supported by evidence. No black holes have been created at RHIC, and none have been created by highly energetic cosmic rays that are hundreds of TeV in energy, which are at least an order of magnitude higher than anything the LHC can ever get to.

Zz.
 
  • #37
Doesn't that theory involve quantum mechanics where anti-particles and particles are randomly created by quantum probability "jitters" that then almost immediately annihilate each other, momentarily making really tiny black holes? Or and I confusing theories with each other?
 

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