Observing a cube approaching a black hole

In summary, the conversation discusses how a distant observer would perceive a large cube approaching a black hole. It is determined that the observer would see the edges of the face become shorter and curved, the center bulging out, and the sides losing their parallel configuration and converging towards the black hole. The effects of the curvature of space and time are also considered, with the conclusion that gravitational time dilation can exist without tidal forces. The concept of gravitational redshift is also mentioned, highlighting the relationship between the relative acceleration of infinitesimally separated worldlines and the Riemann curvature tensor.
  • #1
EskWIRED
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If a distant observer were to observe a large cube made of strong material approach a black hole, what would he see?

ISTM that if one of the faces of the cube were to be the nearest approaching portion, he would see the four edges of the face become shorter and curved, and he would see the center of the face bulge out. ISTM that he would also see the sides of the cube lose their parallel configuration, and that they would converge in the direction of the black hole.

Is that correct? Or would the curvature of time affect what he sees in addition to the effects of the curvature of space?
 
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  • #2
It would depend on the size of the BH. For a small one, spaghettification would occur far enough outside the event horizon that the remote observer would see it and your scenario would not be correct.

For a really big one, your scenario might be correct --- I don't know.
 
  • #3
Here's a discussion of the Special Relativistic effects on the appearance of a moving cube.
 
  • #4
EskWIRED said:
ISTM that if one of the faces of the cube were to be the nearest approaching portion, he would see the four edges of the face become shorter and curved, and he would see the center of the face bulge out. ISTM that he would also see the sides of the cube lose their parallel configuration, and that they would converge in the direction of the black hole.

I'm not sure why you think this would happen. For one thing, I'm not sure if you think these are actual effects on the cube (i.e., an observer near the cube would see them too), or if you think they are optical effects due to the way light paths are distorted on their way out to the distant observer.

As far as actual, local effects on the cube, there aren't any unless tidal gravity is strong enough to be significant on the length scale of the cube. If we assume the hole is large enough that that isn't the case, then an observer near the cube would see it as a normal cube.

As far as distortion of light paths, I have not worked through that in detail, but I think it would depend on where the distant observer was. If the observer is directly above the cube, I don't think there would be any optical effects (except for apparent time dilation, see below). If the observer was looking "from the side", there might be other effects, but I'm not sure they would be similar to those you describe.

EskWIRED said:
Or would the curvature of time affect what he sees in addition to the effects of the curvature of space?

If by "curvature of time" you mean, would the observer see the cube appear to slow down as it falls, yes, he would. But I don't think that would change the apparent shape of the cube.

For "effects of curvature of space", as above, I don't think there are any on the cube itself, but there might be on the paths of light rays.
 
  • #5
PeterDonis said:
If by "curvature of time" you mean, would the observer see the cube appear to slow down as it falls, yes, he would. But I don't think that would change the apparent shape of the cube.
Isn't the effect of falling itself and tidal forces related to gravitational time dilation ("curvature of time").

PeterDonis said:
For "effects of curvature of space", as above, I don't think there are any on the cube itself, but there might be on the paths of light rays.
If you build a large rigid 3D object in flat space and move it into curved space, wouldn't it break?
 
  • #7
A.T. said:
Isn't the effect of falling itself and tidal forces related to gravitational time dilation ("curvature of time").

You can have gravitational time dilation without any tidal forces (vanishing space-time curvature); take for example Rindler space-time.
 
  • #8
WannabeNewton said:
You can have gravitational time dilation without any tidal forces (vanishing space-time curvature); take for example Rindler space-time.
Never suggested otherwise. And here we talk about a black hole.
 
  • #9
A.T. said:
Never suggested otherwise. And here we talk about a black hole.

The point is that there is no relation. What relation is there between tidal forces and gravitational time dilation if one can exist without the other? The derivation of the gravitational time dilation formula between two static observers (and their clocks) in stationary space-times makes no reference to tidal forces.
 
  • #10
WannabeNewton said:
What relation is there between tidal forces and gravitational time dilation if one can exist without the other?
Can tidal forces exist without gravitational time dilation?
 
  • #11
No but that doesn't imply there is a relationship between them; again, gravitational time dilation can exist without tidal forces. Can you derive a formula relating the two? Physically, gravitational time dilation depends upon the inertial/non-inertial states of the two observers involved; the gravitational field of course affects what constitutes an inertial/non-inertial frame. Consider the intimately related but more "intuitive" concept of gravitational redshift: when a light ray is emitted by a static observer and received by another static observer at a different altitude in a static gravitational field, the receiving static observer measures a frequency shift but if the receiving observer is freely falling then no frequency shift will be observed. How is this related to tidal forces, which involves the relationship between the relative acceleration of infinitesimally separated worldlines in a time-like congruence and the Riemann curvature tensor?
 
  • #12
WannabeNewton said:
No but that doesn't imply there is a relationship between them
If tidal forces cannot exist without gravitational time dilation, doesn't that imply some dependency?

WannabeNewton said:
gravitational time dilation can exist without tidal forces.
Does this preclude a relationship? In differential relationships a derivative might vanish in some special cases.
 
  • #13
A.T. said:
If tidal forces cannot exist without gravitational time dilation, doesn't that imply some dependency?

The only dependency is that if tidal forces exist then the space-time is curved and in curved space-time, gravitational time dilation can be observed in an observer dependent sense. There is no implication just from this that tidal forces and gravitational time dilation have any direct relationship.

A.T. said:
Does this preclude a relationship? In differential relationships a derivative might vanish in some special cases.

That is true but the case here is different: we can talk about gravitational time dilation without any need for tidal forces in full generality, not just in special cases.

I assume you have a good physical reason for why you believe tidal forces and gravitational time dilation are directly related. What is your reasoning? I'm not saying that I'm absolutely right and that you're unequivocally wrong, hence seeing your reasoning would help fine tune the discussion. Keep in mind that you can (for example) transform away the effect of gravitational redshift in a freely falling frame but you cannot transform away the Riemann curvature tensor in a freely falling frame.
 

1. How does time dilation affect the appearance of a cube approaching a black hole?

As the cube gets closer to the black hole, the intense gravitational pull causes time to slow down. This means that from an observer's perspective, the cube will appear to move slower and slower as it approaches the black hole.

2. Will the cube actually reach the event horizon of the black hole?

It is possible for the cube to reach the event horizon, which is the point of no return for anything entering a black hole. However, if the cube is approaching a supermassive black hole, it may simply be pulled apart by the immense tidal forces before reaching the event horizon.

3. Can we observe the effects of gravitational lensing on the cube as it approaches the black hole?

Yes, as the cube gets closer to the black hole, the intense gravity will cause light to bend around it, creating a distorted image of the cube known as gravitational lensing. This effect can be observed by telescopes on Earth.

4. How does the shape of the cube change as it nears the black hole?

The intense tidal forces near a black hole can cause objects to elongate in the direction of the black hole's pull. This means that the cube may appear to be stretched or squished as it gets closer to the black hole.

5. What happens to the cube once it enters the black hole?

Once the cube crosses the event horizon, it will continue to be pulled towards the center of the black hole, known as the singularity. At this point, the cube will be crushed into an infinitely small point of infinite density, known as a gravitational singularity.

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