On the nature of the infinite fall toward the EH

  • #401


zonde said:
I can evaluate if prediction is scientifically testable even without knowing how it was derived.
Yes, but if you don't understand how it was derived then you don't understand under what conditions it is logically implied by the things that have been tested.

Furthermore, that objection doesn't apply to event horizons. The predictions about what happens at the horizon can be tested. Signals from the test cannot reach us here since we are outside its future light cone, but we are also outside the future light cone of many other experiments of things that I am sure you would agree are testable.

zonde said:
There is observer A who is using coordinate system K and there is observer B who is using coordinate system K'. Now observer A observes event X but observer B observes event X'. How do they find out if event X and event X' is the same event?
They transform one coordinate to the other chart.

zonde said:
Degeneracy of matter.
And what would cause matter to become degenerate at the horizon?
 
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  • #402


DaleSpam said:
Yes, but if you don't understand how it was derived then you don't understand under what [STRIKE]conditions[/STRIKE] assumptions it is logically implied by the things that have been tested.
My replacement.

Now the way I wrote it, if we can't test prediction we can't find out if assumptions hold. But if we can't find out that then the derivation is not very interesting.

DaleSpam said:
Furthermore, that objection doesn't apply to event horizons. The predictions about what happens at the horizon can be tested. Signals from the test cannot reach us here since we are outside its future light cone, but we are also outside the future light cone of many other experiments of things that I am sure you would agree are testable.
Test is when we do something and then we learn something about the thing we did.
It's action and feedback. If you leave out feedback (or learning) part it's not a test.

DaleSpam said:
They transform one coordinate to the other chart.
And then you compare coordinates of two events, right? You identify events by their coordinates. So you can't get away just by using invariants.

DaleSpam said:
And what would cause matter to become degenerate at the horizon?
You are begging the question. If we talk about event horizon then we imply that BH can form as a result of runaway gravitational collapse. So there is no point asking what will prevent runaway gravitational collapse.
 
  • #403


zonde said:
You identify events by their coordinates.

No, you identify events by what happens at them, and what happens at them is expressed in terms of invariants. You can express those invariants without even choosing a coordinate chart; coordinate charts are a convenience, not a necessity.
 
  • #404


zonde said:
My replacement.

Now the way I wrote it, if we can't test prediction we can't find out if assumptions hold. But if we can't find out that then the derivation is not very interesting.
I am fine with that replacement. It doesn't change my point any.

For example, I can have direct evidence of the value of the fine structure constant from my lab today, and I can have direct evidence of the value of the fine structure constant from your lab yesterday, since signals from both experiments can reach me here and now. I cannot have any direct evidence of the value of the fine structure constant in my lab tomorrow because a signal from such an experiment cannot possibly reach me here and now.

However, if I assume that the laws of physics are homogenous then the value of the fine structure constant in my lab tomorrow is logically implied by that assumption and the experimental evidence of its value here today and there yesterday. Furthermore, while we cannot gather any direct evidence of its value here tomorrow we can design experiments that would be sensitive to violations in our assumption of homogeneity. Taken together those can give us strong empirical evidence of something for which we cannot gather data.

Similarly for the event horizon. In this case the assumption is the Einstein equivalence principle. That and all the rest of the laws of physics as we know them imply that events at and beyond the horizon do exist. The evidence that we have supporting GR and the standard model as well as the evidence we have supporting the Einstein equivalence principle, taken together, are good evidence for the existence of the interior of the EH.

zonde said:
Test is when we do something and then we learn something about the thing we did.
It's action and feedback. If you leave out feedback (or learning) part it's not a test.
Yes, I understand that, and was assuming that. Even with that restriction predictions about what happens at the horizon can be tested. You can learn about the tests at and beyond the horizon as long as you are at or beyond the horizon yourself.

zonde said:
And then you compare coordinates of two events, right? You identify events by their coordinates. So you can't get away just by using invariants.
Sure you can. Coordinates are not the only way to identify events. Events are more primitive than coordinates, they are points in the manifold, i.e. geometric objects independent of coordinates.

zonde said:
You are begging the question. If we talk about event horizon then we imply that BH can form as a result of runaway gravitational collapse. So there is no point asking what will prevent runaway gravitational collapse.
You are correct, I was begging the question of the existence of the horizon. However, I was not trying to ask about the horizon but about your claim regarding degeneracy, so let me rephrase:

And what would cause matter to become degenerate during gravitational collapse and prevent a horizon from forming?
 
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  • #405


DaleSpam said:
I am fine with that replacement. It doesn't change my point any.

For example, I can have direct evidence of the value of the fine structure constant from my lab today, and I can have direct evidence of the value of the fine structure constant from your lab yesterday, since signals from both experiments can reach me here and now. I cannot have any direct evidence of the value of the fine structure constant in my lab tomorrow because a signal from such an experiment cannot possibly reach me here and now.

However, if I assume that the laws of physics are homogenous then the value of the fine structure constant in my lab tomorrow is logically implied by that assumption and the experimental evidence of its value here today and there yesterday. Furthermore, while we cannot gather any direct evidence of its value here tomorrow we can design experiments that would be sensitive to violations in our assumption of homogeneity. Taken together those can give us strong empirical evidence of something for which we cannot gather data.

Similarly for the event horizon. In this case the assumption is the Einstein equivalence principle. That and all the rest of the laws of physics as we know them imply that events at and beyond the horizon do exist. The evidence that we have supporting GR and the standard model as well as the evidence we have supporting the Einstein equivalence principle, taken together, are good evidence for the existence of the interior of the EH.
So basically your argument is that it is not reasonable to expect sudden breakdown of equivalence principle. So if we test equivalence principle to further and further limits and it holds just as well then our confidence grows that it won't break at even further limits, right?

DaleSpam said:
Yes, I understand that, and was assuming that. Even with that restriction predictions about what happens at the horizon can be tested. You can learn about the tests at and beyond the horizon as long as you are at or beyond the horizon yourself.
Hmm, let me rephrase my statement. We can't falsify prediction of event horizon. If prediction about event horizon is false then we of course can't appear at event horizon.

And more down to Earth objection to that. I am not sure it is a valid test when an experimenter should become part of the experimental setup. Say we can reason that it is possible to test if there is life after death - just kill yourself and you will find out.

DaleSpam said:
Sure you can. Coordinates are not the only way to identify events. Events are more primitive than coordinates, they are points in the manifold, i.e. geometric objects independent of coordinates.
Yes, events are more primitive than coordinates. But how does this make a point about invariants identifying events?

And I want to add that while we might try to identify events by other means than coordinates we can uniquely identify events only by coordinates.

For example, when you write a paper you put at the end references. And references are expressed as when and where the paper was published. Even title is optional. Well we have one invariant - name of the author. But it would be possible to find the paper even without the author.

DaleSpam said:
And what would cause matter to become degenerate during gravitational collapse and prevent a horizon from forming?
It's just an observation that there is such a thing. Well I have some speculations about the cause but I am not sure you want to know them as I suppose you want arguments not explanations. And in that case it goes as far as observations.
 
  • #406


zonde said:
So basically your argument is that it is not reasonable to expect sudden breakdown of equivalence principle. So if we test equivalence principle to further and further limits and it holds just as well then our confidence grows that it won't break at even further limits, right?
Yes. We have physical laws that have been tested to reasonable levels of accuracy (GR and SM) and we have an assumption that has also been tested to reasonable levels of accuracy (EEP). Together they imply the existence of events on the horizon and inside. It certainly is possible that further testing will falsify one or more of those, but until such tests are available, the position with the best empirical support is the standard one.

In order to believe otherwise you must reject an assumption or a law for which we currently have empirical support and insert an alternative law or assumption for which we do not have any specific empirical support.

zonde said:
Hmm, let me rephrase my statement. We can't falsify prediction of event horizon. If prediction about event horizon is false then we of course can't appear at event horizon.
True, but we could falsify GR's prediction of a horizon. If the horizon doesn't behave exactly how GR says it does then GR's prediction is falsified. It is true that we could always make a different theory with horizons elsewhere, but it wouldn't be GR as we know it.

zonde said:
And more down to Earth objection to that. I am not sure it is a valid test when an experimenter should become part of the experimental setup. Say we can reason that it is possible to test if there is life after death - just kill yourself and you will find out.
I think that is a valid test for life after death. But, since I will eventually have that test forced upon me, I personally am not inclined to pursue it further at this time :smile:

However, I don't think that tests of the EH fall into that same category. I.e. I would assume that the experimental test for the EH would involve some clocks and some signal receivers and emitters and perhaps some devices to measure tidal gravity. The experimenter wouldn't be any part of that. But, as with all experiments, in order to learn about the outcome the experimenter must be in the future light cone of the experiment. That requires crossing the EH also.

zonde said:
And I want to add that while we might try to identify events by other means than coordinates we can uniquely identify events only by coordinates.
There is only one event on the worldline of the center of my watch where its proper time reads 12:48 pm Dec. 22, 2012. That event is uniquely identified by the invariant description just given (specified worldline and specified proper time).

zonde said:
It's just an observation that there is such a thing. Well I have some speculations about the cause but I am not sure you want to know them as I suppose you want arguments not explanations. And in that case it goes as far as observations.
So there is no empirical support for your position. You just have an aesthetic aversion to the idea of an EH and so, since it doesn't sit well with you, you are just making stuff up.

Btw, matter degeneracy won't stop the horizon from forming. It may be degenerate, but as long as it has mass it will curve spacetime.
 
  • #407


DaleSpam said:
So there is no empirical support for your position. You just have an aesthetic aversion to the idea of an EH and so, since it doesn't sit well with you, you are just making stuff up.
Well as I know at least electrons in metals are degenerate.
From wikipedia article about Fermi-Dirac statistics:
"Before the introduction of Fermi–Dirac statistics in 1926, understanding some aspects of electron behavior was difficult due to seemingly contradictory phenomena. For example, the electronic heat capacity of a metal at room temperature seemed to come from 100 times fewer electrons than were in the electric current.[3] It was also difficult to understand why the emission currents, generated by applying high electric fields to metals at room temperature, were almost independent of temperature."

But usually degeneracy of matter is modeled as pressure and that does not seem quite right to me.
See here - Degenerate matter
 
  • #408


Again, how would degeneracy do anything to prevent a horizon. Degeneracy doesn't magically make any mass or energy disappear, so the curvature will remain.
 
  • #409


zonde said:
But usually degeneracy of matter is modeled as pressure and that does not seem quite right to me.

What else would you model it as? It's true that degeneracy pressure doesn't arise kinetically (i.e., it's independent of temperature), but so what? The effect at the classical level is the same: the material resists being compressed. That's what "pressure" is, from the standpoint of the stress-energy tensor: resistance to compression.
 
  • #410


Quote by Austin0 View Post

Yes their coordinate velocity is reducing but in the Zeno system a la Pervect there is no reason that Achilles proper velocity would not also decrease.

DaleSpam said:
Achilles' proper velocity is clearly constant.
.
DaleSpam said:
I can calculate it explicitly if you like, but it is exceedingly well-founded.
Achilles' proper velocity is clearly constant.
.

Quote by Austin0 View Post

Yes this is fine . But it is based on an assumption of a constant v in Achilles' frame ,,,,yes?


DaleSpam said:
Yes, that is a standard part of Zeno's paradox. See the second sentence of the description here:

http://en.wikipedia.org/wiki/Zeno's_...d_the_tortoise .

SO it appears that your assertion that Achilles velocity is constant is based, not on calculation, but on your interpretation of the explicit statements of the classical scenario...yes? Yes I am aware it is a part of the classical paradox as I mentioned in my initial post

Austin0 said:
In the first case (Zeno) as the distance incrementally reduces, the velocity of Achilles remains constant. So for each reduction in distance, the time for the next reduction in distance becomes shorter.
.

But in the classical statement it is evident that the stated constant velocity is in the
frame of the ground. I.e. Zeno coordinates.
Do you disagree? What other possible frame for such a statement do you propose?

So when Pervect redefines Achilles velocity as non-uniform in the Zeno frame it is now ,not necessarily a logical conclusion that Achilles velocity is constant in any other frame, as no other frame was defined .


DaleSpam said:
In Zeno coordinate time the time for the next reduction is constant, by definition. So the Zeno coordinate velocity in fact reduces.

It is the proper time which reduces. And the velocity in some unspecified inertial coordinate system which remains constant..

According to Pervect's explicit description it seems to follow that the Zeno coordinate system is not accelerating. That it would be in a state of uniform motion relative to and measured by any inertial frame. Do you disagree??

So if Achilles is in non- uniform motion (accelerating) as measured in the Zeno frame how do you propose that it is measured as uniform (inertial) in anyone of those other inertial frames?

So what is the basis ,in the classical description, for your assumption of constant velocity for Achilles ?

What unspecified inertial frame ?

Without a valid basis for an assumption of constant velocity there is no basis for calculating a different time rate for Achilles either, is there?

DaleSpam said:
Saying that it added nothing is one thing, but saying it is misleading is accusatory and untrue. It is, as I think is now established, a valid and close analogy in many respects. The fact that the parallels escaped you at first doesn't make it misleading or deceptive in any way.

It was not that the parallels escaped me or the math was too complex it was purely a question of logic and applicability.
I certainly never thought for a moment there was deception on Pervects part.

OTOH wouldn't you agree that the original is easily and unambiguously falsified by empirical demonstration? As simple as getting up and catching up to a friend.

Wouldn't you also agree that creating an association between the two cases seems to imply that the Sc case is equally unambiguously false??

But isn't the amended Zeno case now as unfalsifiable in the real world as the Sc scenario?
As ambiguous??
Do you think that if Achilles started out in Zeno's time with Pervect's conditions he would have caught the tortoise by now in our frame (Zeno coordinates)??
 
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  • #411


DaleSpam said:
Again, how would degeneracy do anything to prevent a horizon. Degeneracy doesn't magically make any mass or energy disappear, so the curvature will remain.
"Degeneracy of matter" does not tell us why it happens. It just tells that it happens.

Look, Pauli exclusion principle says that no two identical fermions can occupy the same quantum state. It does not tell us what would happen if two identical fermions would try to occupy the same quantum state. Currently we have no idea why the nature behaves that way.

And there is still some room for interpretation. QM gives quite abstract definition for "quantum state". From wikipedia article about quantum state:
"In quantum physics, quantum state refers to the state of a quantum system. A quantum state is given as a vector in a vector space, called the state vector."

Well, we consider particles to be physical entities but quantum state is defined as mathematical entity. So it seems that Pauli exclusion principle is not very rigorous. This leaves (at least for me) the question open how we should model quantum state in real space (space-time).
 
  • #412


PeterDonis said:
What else would you model it as? It's true that degeneracy pressure doesn't arise kinetically (i.e., it's independent of temperature), but so what? The effect at the classical level is the same: the material resists being compressed. That's what "pressure" is, from the standpoint of the stress-energy tensor: resistance to compression.
I would model it as a slipping away from the trap and not as a resistance to the trap. Let's say it this way - degenerate matter can not be contained.
 
  • #413


zonde said:
"Degeneracy of matter" does not tell us why it happens. It just tells that it happens.

Look, Pauli exclusion principle says that no two identical fermions can occupy the same quantum state. It does not tell us what would happen if two identical fermions would try to occupy the same quantum state. Currently we have no idea why the nature behaves that way.

And there is still some room for interpretation. QM gives quite abstract definition for "quantum state". From wikipedia article about quantum state:
"In quantum physics, quantum state refers to the state of a quantum system. A quantum state is given as a vector in a vector space, called the state vector."

Well, we consider particles to be physical entities but quantum state is defined as mathematical entity. So it seems that Pauli exclusion principle is not very rigorous. This leaves (at least for me) the question open how we should model quantum state in real space (space-time).
OK. I am fine with all of this, but I am still missing the connection with how any of this prevents the formation of the EH. I could see it preventing the formation of the singularity, but not the horizon.
 
  • #414


Austin0 said:
SO it appears that your assertion that Achilles velocity is constant is based, not on calculation, but on your interpretation of the explicit statements of the classical scenario...yes?
Yes.

Austin0 said:
But in the classical statement it is evident that the stated constant velocity is in the frame of the ground. I.e. Zeno coordinates.
I don't think that the "classical statement" ever explicitly introduced any coordinates. That was pervect's idea, taking the familiar statement of Zeno's paradox and using it to define a coordinate time. So I would not associate Zeno coordinates with the frame of the ground since "frame of the ground" usually indicates an inertial frame and Zeno coordinats are non-inertial.

Austin0 said:
Do you disagree? What other possible frame for such a statement do you propose?
Any inertial frame. If it is true in one inertial frame then it is true in all.

Austin0 said:
So when Pervect redefines Achilles velocity as non-uniform in the Zeno frame it is now ,not necessarily a logical conclusion that Achilles velocity is constant in any other frame, as no other frame was defined .
Achilles motion is inertial. That is an invariant fact which is true in all coordinate systems and does not change with pervect's introduction of Zeno coordinates. Given that his motion is inertial (frame invariant) then his velocity (frame variant) is constant in any inertial frame.

Austin0 said:
According to Pervect's explicit description it seems to follow that the Zeno coordinate system is not accelerating. That it would be in a state of uniform motion relative to and measured by any inertial frame. Do you disagree??
Yes, I disagree quite strongly. The Zeno coordinate system is decidedly non-inertial. In fact, from my post 393 you can easily see that the metric in the Zeno coordinates is:
ds^2=-c^2 \left( \frac{(100-vt) ln(2)}{v} \right)^2 dn^2 + dx^2 + dy^2 + dz^2

This metric is clearly different from the metric in an inertial frame.

Austin0 said:
So if Achilles is in non- uniform motion (accelerating) as measured in the Zeno frame how do you propose that it is measured as uniform (inertial) in anyone of those other inertial frames?
Again, his motion is inertial in all frames, that is an invariant which follows directly from the original description and is not changed by the introduction of any coordinate system. The Zeno coordinates are non-inertial and therefore it is no surprise that he is accelerating in the Zeno frame and not accelerating in any inertial frame.

Austin0 said:
OTOH wouldn't you agree that the original is easily and unambiguously falsified by empirical demonstration? As simple as getting up and catching up to a friend.

Wouldn't you also agree that creating an association between the two cases seems to imply that the Sc case is equally unambiguously false??
Yes, that is the whole point of the analogy.

However, let's be careful about exactly the way in which the original is false. The original is correct in its description of all events up to (but not including) the event where Achilles catches up with the turtle. Where it fails is if it asserts anything about events at or beyond that point. Similarly with SC, SC is correct in its description of all events up to (but not including) the EH. Where it fails is if it asserts anything about events at or beyond the EH.
 
  • #415


zonde said:
"Degeneracy of matter" does not tell us why it happens. It just tells that it happens.

Look, Pauli exclusion principle says that no two identical fermions can occupy the same quantum state. It does not tell us what would happen if two identical fermions would try to occupy the same quantum state. Currently we have no idea why the nature behaves that way.

I don't understand why degeneracy would have any relevance to black hole event horizons. Are you thinking that matter falling toward the event horizon would run out of states, and so the Pauli exclusion principle would prevent a collection of Fermions from falling further? If that's what you're thinking, then that's not correct. Nothing special happens at the event horizon that would force matter to become degenerate.
 
  • #416


zonde said:
"Degeneracy of matter" does not tell us why it happens. It just tells that it happens.

Look, Pauli exclusion principle says that no two identical fermions can occupy the same quantum state. It does not tell us what would happen if two identical fermions would try to occupy the same quantum state. Currently we have no idea why the nature behaves that way.

And there is still some room for interpretation. QM gives quite abstract definition for "quantum state". From wikipedia article about quantum state:
"In quantum physics, quantum state refers to the state of a quantum system. A quantum state is given as a vector in a vector space, called the state vector."

Well, we consider particles to be physical entities but quantum state is defined as mathematical entity. So it seems that Pauli exclusion principle is not very rigorous. This leaves (at least for me) the question open how we should model quantum state in real space (space-time).

What does any of this have to do with horizon formation for millions of galactic center BH, each with mass of millions to billions of suns. The issue here is that matter density for the aggregate at SC radius is much less than stellar atmosphere density, let alone stellar centers or neutron stars. How does degeneracy even become relevant?
 
  • #417


zonde said:
Well, we consider particles to be physical entities but quantum state is defined as mathematical entity. So it seems that Pauli exclusion principle is not very rigorous. This leaves (at least for me) the question open how we should model quantum state in real space (space-time).

Quantum states *are* modeled using real spacetime; spacetime position is part of the description of a quantum state. The Pauli exclusion principle does not prevent two fermions of the same particle type from being in the same spin state at two different spacetime positions; it only prevents two fermions of the same particle type from being in the same spin state at the *same* spacetime position.

Actually, even that is not really the right way to say it. The Pauli exclusion principle as we have stated it is not a fundamental law; the fundamental law is that fermion wave functions are antisymmetric under particle exchange, whereas boson wave functions are symmetric. If I have a boson, say a spin-0 particle, at spacetime position x, and another spin-0 particle of the same particle type at spacetime position y, the wave function is symmetric under exchange of those two particles. But if I have a fermion in a definite spin state, say a spin-up electron, at spacetime position x, and another spin-up electron at spacetime position y, the wave function is antisymmetric (i.e., it changes sign) under exchange of those two particles.

The Pauli exclusion principle, which says that the wave function is identically zero if x = y, is an obvious consequence of the antisymmetry. However, it's not the only consequence; another consequence is that as x and y get closer together, the amplitude of the wave function decreases. That's what causes degeneracy pressure.

But all of that is below the level that GR models anyway. GR doesn't care about the microscopic details of matter; all it cares about is the stress-energy tensor. Degeneracy pressure, from the standpoint of the stress-energy tensor, works just like any other kind of pressure. The only real difference is the equation of state, i.e., the relationship between pressure and energy density.
 
  • #418


DaleSpam said:
OK. I am fine with all of this, but I am still missing the connection with how any of this prevents the formation of the EH. I could see it preventing the formation of the singularity, but not the horizon.
Formation of EH relies on idea that gravitating object can get more compact without any change to physical laws. But degeneracy of matter becomes more important at more compact configurations of matter.

PAllen said:
What does any of this have to do with horizon formation for millions of galactic center BH, each with mass of millions to billions of suns. The issue here is that matter density for the aggregate at SC radius is much less than stellar atmosphere density, let alone stellar centers or neutron stars. How does degeneracy even become relevant?
To discuss scenario like this we would have to have some idea how we would model occupied and available quantum states as we add more particles to given ensemble of particles. Or what happens with occupied and available quantum states as two ensembles of degenerate matter approach each other.

Your assumptions seems to be that particles affect occupancy of quantum levels only over short distance.
I assume that occupancy of quantum level drops as inverse square law as we go further from the particle.
 
  • #419


stevendaryl said:
I don't understand why degeneracy would have any relevance to black hole event horizons. Are you thinking that matter falling toward the event horizon would run out of states, and so the Pauli exclusion principle would prevent a collection of Fermions from falling further? If that's what you're thinking, then that's not correct. Nothing special happens at the event horizon that would force matter to become degenerate.
I suggest you to reformulate your question. Because there is a problem with it as it is stated. As you refer to pre-existing event horizon you imply that it is formed as a result of runaway gravitational collapse i.e. you are begging the question. I already raised the issue in post #402. So DaleSpam agreed that we should talk about hypothetical formation of event horizon instead.
 
  • #420


zonde said:
Formation of EH relies on idea that gravitating object can get more compact without any change to physical laws. But degeneracy of matter becomes more important at more compact configurations of matter.
This is relevant for the formation of the singularity, not for the formation of the EH. The singularity is an infinitely dense object, but an EH can form at arbitrarily low densities. For example, see Susskind's 12th lecture on GR () from about 2:00 to about 2:03 (of course the whole series is good).

I.e. your assumption "Formation of EH relies on idea that gravitating object can get more compact" is not correct. The formation of the singularity relies on that, but not the EH. The EH can form with simply a very large amount of non-compact material and you do not need a singularity in order to obtain an EH.

So again, what would prevent the formation of the EH? Degeneracy won't do it, that would only prevent the formation of the singularity.
 
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  • #421


zonde said:
To discuss scenario like this we would have to have some idea how we would model occupied and available quantum states as we add more particles to given ensemble of particles. Or what happens with occupied and available quantum states as two ensembles of degenerate matter approach each other.

Your assumptions seems to be that particles affect occupancy of quantum levels only over short distance.
I assume that occupancy of quantum level drops as inverse square law as we go further from the particle.

So we have new fundamental law of physics: the "stellar exclusion principle" that prevents gathering too many stars in the same large region??! Remember, the EH forms before there is any singularity or even any high density anywhere in the formative collapsing mass.
 
  • #422


zonde said:
Your assumptions seems to be that particles affect occupancy of quantum levels only over short distance.
I assume that occupancy of quantum level drops as inverse square law as we go further from the particle.

So you're saying that quantum effects play a non-negligible part in the dynamics of stars that are separated by light-years? That, for example, quantum interactions between the Sun and Alpha Centauri affect the relative motion of those two stars?
 
  • #423


DaleSpam said:
This is relevant for the formation of the singularity, not for the formation of the EH. The singularity is an infinitely dense object, but an EH can form at arbitrarily low densities. For example, see Susskind's 12th lecture on GR () from about 2:00 to about 2:03 (of course the whole series is good).

I.e. your assumption "Formation of EH relies on idea that gravitating object can get more compact" is not correct. The formation of the singularity relies on that, but not the EH. The EH can form with simply a very large amount of non-compact material and you do not need a singularity in order to obtain an EH.

So again, what would prevent the formation of the EH? Degeneracy won't do it, that would only prevent the formation of the singularity.

There are two ways how to arrive at situation where EH is supposed to form.
First, we can add more matter to given gravitating object while it's radius is not increased too much by this addition.
Second, we can make given gravitating object more compact while it's mass is not reduced too much by this compactification.

I guessed that you was talking about the second scenario. If you are considering first scenario and want arguments concerning this scenario in particular please say it so that I don't have to guess.
 
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  • #424


PAllen said:
So we have new fundamental law of physics: the "stellar exclusion principle" that prevents gathering too many stars in the same large region??! Remember, the EH forms before there is any singularity or even any high density anywhere in the formative collapsing mass.
New? Why new? I am just extrapolating existing law.
 
  • #425


PeterDonis said:
So you're saying that quantum effects play a non-negligible part in the dynamics of stars that are separated by light-years? That, for example, quantum interactions between the Sun and Alpha Centauri affect the relative motion of those two stars?
No, I am not talking about dynamics of stars but about dynamics of particles.
So what I say is that if we have two fairly degenerate stars approaching each other then whey would melt first and after that will start to evaporate. Or alternatively will fall into pieces depending on homogeneity of star.

If particles can't remain in their quantum states they can't maintain their collective structure. Kind of obvious IMO.
 
  • #426


zonde said:
I guessed that you was talking about the second scenario. If you are considering first scenario and want arguments concerning this scenario in particular please say it so that I don't have to guess.
I am considering any scenario where an EH forms. If there are multiple ways for an EH to form then a mechanism for preventing EH formation has to prevent all of them.

In general an EH forms whenever there is enough mass inside the Schwarzschild radius. That can happen at any density, so a mechanism which prevents high densities, like degeneracy, simply cannot prevent EH formation in general.
 
  • #427


zonde said:
I suggest you to reformulate your question. Because there is a problem with it as it is stated. As you refer to pre-existing event horizon you imply that it is formed as a result of runaway gravitational collapse i.e. you are begging the question. I already raised the issue in post #402. So DaleSpam agreed that we should talk about hypothetical formation of event horizon instead.

I'm not begging the question. I'm asking you a question. Why do you believe that degeneracy has anything to do with the formation of an event horizon? You can certainly make up your own theory, but there is nothing in General Relativity that would suggest that. If you're not talking about General Relativity, then what are you talking about?
 
  • #428


zonde said:
No, I am not talking about dynamics of stars but about dynamics of particles.
So what I say is that if we have two fairly degenerate stars approaching each other then whey would melt first and after that will start to evaporate. Or alternatively will fall into pieces depending on homogeneity of star.

If particles can't remain in their quantum states they can't maintain their collective structure. Kind of obvious IMO.

If you are making up your own theory of gravity, then I think this is not the appropriate place to talk about it. If you are talking about mainstream physics, then it is well understood that degeneracy prevents further collapse for any star less massive than the Chandrasekhar limit (described here: http://en.wikipedia.org/wiki/Chandrasekhar_Limit).
 
  • #429


stevendaryl said:
it is well understood that degeneracy prevents further collapse for any star less massive than the Chandrasekhar limit (described here: http://en.wikipedia.org/wiki/Chandrasekhar_Limit).

Small technical point: the Chandrasekhar limit applies to white dwarfs, i.e., to objects in which electron degeneracy is the primary mechanism resisting compression. The analogous limit for neutron stars, where neutron degeneracy is the primary mechanism, is the Tolman-Oppenheimer-Volkoff limit:

http://en.wikipedia.org/wiki/Tolman–Oppenheimer–Volkoff_limit

Conceptually, both limits work the same, but the details are different because of the different types of fermions involved (neutrons vs. electrons).
 
  • #430


zonde said:
So what I say is that if we have two fairly degenerate stars approaching each other then whey would melt first and after that will start to evaporate. Or alternatively will fall into pieces depending on homogeneity of star.

Do you have any actual argument for why this would happen? Why would a degenerate star suddenly start melting? If the two degenerate stars collide with each other, then I could see matter being ejected from the collision; but if the stars are just free-falling towards each other, what difference would that make to their internal structure? The quantum states inside the star don't "know" that the two stars are approaching each other, unless they actually collide.
 
  • #431


zonde said:
Formation of EH relies on idea that gravitating object can get more compact without any change to physical laws.

Huh? This makes no sense. The physical laws involved are the Einstein Field Equation and the equation of state for the matter. It is well known that there are a range of reasonable equations of state that allow a gravitating object to get compact enough to form an EH; there are both analytical solutions and numerical simulations that show this. The laws certainly don't need to "change" at any point during the process.
 
  • #432


zonde said:
As you refer to pre-existing event horizon you imply that it is formed as a result of runaway gravitational collapse i.e. you are begging the question

Since there are already known solutions of the EFE with various equations of state that show runaway gravitational collapse, assuming it is possible is not begging the question.
 
  • #433


PeterDonis said:
Since there are already known solutions of the EFE with various equations of state that show runaway gravitational collapse, assuming it is possible is not begging the question.
I think that he is objecting to the equations of state, in which case it is begging the question. However, I think it is clear that his proposed patch to the equations of state does not accomplish his goal, and since many equations of state lead to an EH it is hard to see that a patch is even possible.
 
  • #434


DaleSpam said:
since many equations of state lead to an EH it is hard to see that a patch is even possible.

Exactly. We don't know enough about the strong nuclear force and QCD to be able to derive the exact equation of state for neutron star matter from first principles, so any equation of state we use is an assumption. We can only debate about which equations of state are "reasonable"; but since as you say, many equations of state lead to an EH forming, it would take a very impressive argument to show that *all* of them are too "unreasonable". I certainly don't see any such argument being made in this thread.
 
  • #435


PeterDonis said:
since as you say, many equations of state lead to an EH forming, it would take a very impressive argument to show that *all* of them are too "unreasonable". I certainly don't see any such argument being made in this thread.
Agreed, particularly for supermassive black holes where the densities required are well within the "ordinary" range in which we have lots of data and experience and very well-validated equations of state.
 
  • #436


DaleSpam said:
Agreed, particularly for supermassive black holes where the densities required are well within the "ordinary" range in which we have lots of data and experience and very well-validated equations of state.

Yes, good point; the neutron star case, where we don't have very good knowledge of the actual equation of state, is only one of many possibilities.
 
  • #437


Quote by Austin0

SO it appears that your assertion that Achilles velocity is constant is based, not on calculation, but on your interpretation of the explicit statements of the classical scenario...yes?

DaleSpam said:
Yes.

Quote by Austin0
But in the classical statement it is evident that the stated constant velocity is in the frame of the ground. I.e. Zeno coordinates.

DaleSpam said:
I don't think that the "classical statement" ever explicitly introduced any coordinates. That was pervect's idea, taking the familiar statement of Zeno's paradox and using it to define a coordinate time. So I would not associate Zeno coordinates with the frame of the ground since "frame of the ground" usually indicates an inertial frame and Zeno coordinats are non-inertial.
Well I agree that Zeno did not explicitly define a coordinate frame ibut he did implicitly define Achilles motion in the terms of the ground.I.e. Achilles successively caught up with a previous position of the tortoise which would naturally be a spatial point on the ground.
So in this context the ground would be an inertial frame. And Pervects statements could validly be interpreted in this context. In which case it would be Achilles motion which was non-inertial.Such an interpretation would be perfectly consistent with Pervects statements right up to total zeno time being infinite. Yes?.
so you are circularly inserting an assumption that Zeno coordinates are non-inertial.

Quote by Austin0

Do you disagree? What other possible frame for such a statement do you propose?

DaleSpam said:
Any inertial frame. If it is true in one inertial frame then it is true in all.

Yes it is possible to assume an interpretation of an abstract unspecified inertial frame however unlikely that was what was assumed by Zeno .
WHich is why I said

Quote by Austin0

So when Pervect redefines Achilles velocity as non-uniform in the Zeno frame it is now ,not necessarily a logical conclusion that Achilles velocity is constant in any other frame, as no other frame was defined .

this.

Clearly I did not suggest that my interpretation was the only possible one but only pointed out that it was also not precluded and other interpretations were not exclusive or preferred.

DaleSpam said:
Achilles motion is inertial. That is an invariant fact which is true in all coordinate systems and does not change with pervect's introduction of Zeno coordinates. Given that his motion is inertial (frame invariant) then his velocity (frame variant) is constant in any inertial frame.

As opposed to your unequivocal statement of "invariant fact" which is actually not the result of inevitable logic but in the end really no more than edict.
Unsupported assertion that my interpretation is wrong and yours is fact.

Quote by Austin0

According to Pervect's explicit description it seems to follow that the Zeno coordinate system is not accelerating. That it would be in a state of uniform motion relative to and measured by any inertial frame. Do you disagree??

DaleSpam said:
Yes, I disagree quite strongly. The Zeno coordinate system is decidedly non-inertial. In fact, from my post 393 you can easily see that the metric in the Zeno coordinates is:

ds^2=-c^2 \left( \frac{(100-vt) ln(2)}{v} \right)^2 dn^2 + dx^2 + dy^2 + dz^2This metric is clearly different from the metric in an inertial frame.

1) this metric is based on your a priori definition of Achilles motion as inertial and Zeno coordinates as non-inertial so is disregarding Pervects description of Achilles non-uniform motion in an inertial system.

2) Could you explain this metric? It is true it does not look like an inertial metric but it also does not resemble the Sc metric either.

If I am understanding it correctly the first term contains both Zeno coordinate time and also Achilles coordinate time yes? How does that work ? it appears a bit circular no??

It also appears that it is based on a constant velocity term in the Zeno frame , how is this possible?

3) What is your definition of inertial.
Lack of accelerometer reading? Disregarding g both Achilles and the Zeno frame are inertial by this standard.

Constant motion. As observed from all inertial frames both Achilles and Zeno frames are in uniform coordinate motion yes? So are equivalent.

As far as I know inertial frames are simply defined by uniform rectilinear motion without explicit reference to time flow so what is your basis for this strong assertion that the Zeno frame is non-inertial?

DaleSpam said:
Consider the inertial frame where Achilles is at rest. In this frame the turtle's worldline is given by (t,100-vt) where v is the relative velocity between Achilles and the turtle. So in this frame Achilles is a distance d=100-vt behind the turtle. The definition of Zeno time, n, given is d=100/2^n. Substituting in and simplifying we get the following transform between the inertial frame and Zeno coordinates:
n=log_2 \left( \frac{100}{100-vt} \right)

Taking the derivative of Zeno coordinate time wrt Achilles proper time we get
\frac{dn}{dt}=\frac{v}{(100-vt) ln(2)} \neq 1
So Achilles' clock does not run at the same rate as Zeno coordinate time.

Taking the inverse transform we get
t=\frac{100}{v}(1-2^{-n})
so
\lim_{n\to \infty } \, t = \frac{100}{v}
So as Zeno coordinate time goes to infinity Achilles proper time does not.

SO as you have declared Achilles motion inertial then it follows that his velocity is constant and time rate uniform so:
your initial premise here d=100-vt means that Achilles catches the tortoise at d=0 or 100-vt=0
so vt=100 and t = \frac{100}{v}

SO clearly yiour conclusion \lim_{n\to \infty } \, t = \frac{100}{v} is directly equivalent to your initial premise [tex t = \frac{100}{v}[/tex] without any of your intermediate steps and is classically circular reasoning. A tautology if you like.

Also: Given your declaration of Achilles inertial motion, as far as I can see there is no possible state of accelerated motion of the Zeno frame that could effectuate the observations of Achilles motion as defined by Pervect.

SO unless you can come up with such a description I propose that Zeno motion is also inertial i.e. constant and the non-uniformity is all temporal. DO you disagree ? If so what possible motion??

In this case then, the temporal non-uniformity could not be actual dilation , meaning change of physical processes etc. as there is no known physics to explain this kind of exponential increase of time rate concurrent with the decrease in coordinate velocity of the inertial Achilles .

SO this leaves arbitrary mechanical clock rate as the only possible scenario consistent with your own conditions and assumptions.

Just as I suggested early on and you rejected with your tautological definition.

Or do you disagree and have an alternative explanation?

so the Zeno clocks speed up exponentially but Zeno observers do not ..

But this seems to me to mean that finite proper time on Achilles clock could not possibly mean infinite time on a mechanically calibrated actual physical clock. SO the analogy is completely non-applicable.

Or do you still disagree?
 
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  • #438


Austin0 said:
Well I agree that Zeno did not explicitly define a coordinate frame ibut he did implicitly define Achilles motion in the terms of the ground.I.e. Achilles successively caught up with a previous position of the tortoise which would naturally be a spatial point on the ground.
So in this context the ground would be an inertial frame. And Pervects statements could validly be interpreted in this context. In which case it would be Achilles motion which was non-inertial.
Again, defining new coordinates does not change any invariants. The fact that Achilles' motion is inertial is an invariant, therefore it cannot change by the introduction of new coordinates. You cannot change the invariants without changing the physics, the scenario.

So, yes, it is an assumption that Achilles' motion is an inertial, that assumption is part of the original well-known scenario. Pervect's definition of a coordinate system does not change that assumption since it is invariant, and an "interpretation" of pervect's comments which assumes that specifying coordinates also changes invriants is simply a mistake.

Austin0 said:
1) this metric is based on your a priori definition of Achilles motion as inertial and Zeno coordinates as non-inertial so is disregarding Pervects description of Achilles non-uniform motion in an inertial system.
You are making a mistake there. Pervect did not make such a description.

Austin0 said:
If I am understanding it correctly the first term contains both Zeno coordinate time and also Achilles coordinate time yes?
Oops, good catch! I definitely missed that. I need to fix that.

Austin0 said:
3) What is your definition of inertial.
Lack of accelerometer reading? Disregarding g both Achilles and the Zeno frame are inertial by this standard.
Yes. That is the standard definition in GR.

EDIT: I later realized that there may be some lingering confusion about the meaning of inertial. When we are talking about a worldline then inertial does mean zero proper acceleration (zero accelerometer reading). When we are talking about a coordinate system then inertial means that the metric is the Minkowski metric in those coordinates. These are both the standard definitions in GR. So Achilles' worldline is inertial under the first definition, and the Zeno coordinates are non-inertial under the second definition. I hadn't originally noticed that you were mixing a worldline and a coordinate system in your question above.

Austin0 said:
what is your basis for this strong assertion that the Zeno frame is non-inertial?
The metric in any inertial frame is the standard Minkowski metric. Of course, I need to fix the metric above in order to show that the time term doesn't simplify to -1.

Austin0 said:
SO clearly yiour conclusion \lim_{n\to \infty } \, t = \frac{100}{v} is directly equivalent to your initial premise [tex t = \frac{100}{v}[/tex] without any of your intermediate steps and is classically circular reasoning. A tautology if you like.
Yes. Which is why pervect and I thought that the analogy was obvious. The coordinate system was explicitly, deliberately, and purposely designed so that that limit would go to infinity as Achillies reached the Tortoise.

Austin0 said:
Also: Given your declaration of Achilles inertial motion, as far as I can see there is no possible state of accelerated motion of the Zeno frame that could effectuate the observations of Achilles motion as defined by Pervect.
I don't know what you mean here. What does "effectuate the observations" mean? Achilles' motion and the Tortoise's motion are inertial, so what accelerated motion are you talking about?

Austin0 said:
In this case then, the temporal non-uniformity could not be actual dilation , meaning change of physical processes etc. as there is no known physics to explain this kind of exponential increase of time rate concurrent with the decrease in coordinate velocity of the inertial Achilles .
What are you talking about here? This is a coordinate system, it is just mathematical labeling, not any physical process nor any physical explanation. That is the point. I don't understand what you mean by "actual dilation" and "change of physical processes"? It seems contrary to the principle of relativity.

Austin0 said:
But this seems to me to mean that finite proper time on Achilles clock could not possibly mean infinite time on a mechanically calibrated actual physical clock. SO the analogy is completely non-applicable.

Or do you still disagree?
I still disagree, the analogy is very close, but I don't understand your most recent objection.
 
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  • #439


Austin0 said:
But this seems to me to mean that finite proper time on Achilles clock could not possibly mean infinite time on a mechanically calibrated actual physical clock. SO the analogy is completely non-applicable.

Or do you still disagree?

I disagree. The analogy with Schwarzschild coordinates is almost exact. In both cases, you have a local inertial coordinate system, according to which it takes a finite amount of time for the traveler to move from point A to point B, and there is a second coordinate system, with a nonlinear relationship to the first, according to which it takes an infinite amount of time for the traveler to move from point A to point B. What are you saying is the difference?

Actually, there is a difference having to do with causality, but it doesn't come into play in anything you've said so far: For the Schwarzschild case, events after the traveler crosses the event horizon are inaccessible to the distant observer, while in the Zeno cases, there are events after Achilles crosses the finish line that are accessible to the distant observer (although they can't be given a time coordinate in the coordinate system of the distant observer).

--
Daryl McCullough
Ithaca, NY
 
  • #440


Austin0 said:
2) Could you explain this metric? It is true it does not look like an inertial metric but it also does not resemble the Sc metric either.
You are correct, it is not the same as the SC metric. The Zeno coordinates are defined on a flat spacetime, so there will always be some difference there. It is an analogy, not a derivation.

Austin0 said:
If I am understanding it correctly the first term contains both Zeno coordinate time and also Achilles coordinate time yes? How does that work ? it appears a bit circular no??
OK, thanks for pointing out my mistake. Unfortunately, it is too late to go and edit the post, so I hope anyone who refers to it in the future notices this update. Anyway, from post 393 we have:
\frac{dn}{dt}=\frac{v}{(100-vt) ln(2)}
and
t=\frac{100}{v}(1-2^{-n})

Substituting the second equation in on the rhs of the first equation and simplifying we get
\frac{dn}{dt}=\frac{2^n v}{100 ln(2)}

So the metric in post 414 should be:
ds^2=-c^2 \left( \frac{100 ln(2)}{2^n v} \right)^2 dn^2 + dx^2 + dy^2 + dz^2

Which again is clearly not the Minkowski metric of an inertial frame, thereby demonstrating that the Zeno coordinates are non-inertial.
 
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  • #441


Quote by Austin0

Also: Given your declaration of Achilles inertial motion, as far as I can see there is no possible state of accelerated motion of the Zeno frame that could effectuate the observations of Achilles motion as defined by Pervect.

DaleSpam said:
I don't know what you mean here. What does "effectuate the observations" mean? Achilles' motion and the Tortoise's motion are inertial, so what accelerated motion are you talking about?

Yes I am referring to the Zeno frame which you have declared is non-inertial (I.e. accelerated).

Pervect has here given a series of events. Or at least relationships as there seems to be no determinable velocities or explicit spatial coordinates to be derived from this information.

Let's define a "zeno time" as follows. At a zeno time of 0, Achillies is 100 meters behind the tortise.

At a zeno time of 1, Achilles is 50 meters behind the tortise.

At a zeno time of 2, Achillies is 25 meters behind the tortise

At a zeno time of n, Achillies is 100/(2^n) meters behind the tortise.

Then, as n goes to infinity, Achillies is always behind the tortise.

So, in "zeno time", Achilles never does catch up with the tortise, even as "zeno time" appoaches infinity.

SO we have these times and relative distances and the premise that both Achilles and the tortoise are inertial with which to synthesize a coordinate system and metric.

You have asserted that the Zeno frame is non-inertial so the question is what possible state of motion of that frame could make possible those observed distances between two bodies in uniform motion.

Maybe an example would help you visualize:
If the observations in the Zeno frame supported a picture of linear decrease in distance between Achilles and the tortoise this would indicate a constant motion of the Zeno frame also , agreed?

If the observed decrease in distance, itself increased in rate , this would support a conclusion of positive parallel acceleration of the Zeno frame.I.e. Zeno frame increasing it's velocity relative to A and the tortoise.

But according to Pervect the decrease in relative distance between Achilles and the tortoise is decreasing over time non-linearly.
SO what possible motion (acceleration) of the Zeno frame could make this possible?

My conclusion is that there is no possible acceleration that could do this alone and therefore the observations in the Zeno frame could only be possible if the Zeno time rate was increasing at a rate not possible through the effects of motion ( Lorentz effects..)

Quote by Austin0

In this case then, the temporal non-uniformity could not be actual dilation , meaning change of physical processes etc. as there is no known physics to explain this kind of exponential increase of time rate concurrent with the decrease in coordinate velocity of the inertial Achilles .

DaleSpam said:
What are you talking about here? This is a coordinate system, it is just mathematical labeling, not any physical process nor any physical explanation. That is the point. I don't understand what you mean by "actual dilation" and "change of physical processes"? It seems contrary to the principle of relativity.

Put simply:
Achilles is passing a stream of Zeno clocks and observers. Do you think Achilles sees everything in the Zeno frame speed up exponentially or only the clocks?

If you think everything speeds up (actual dilation) then what is your explanation of the physics behind this?
This would be to a certain extent possible if Achilles and the tortoise were racing at relativistic speeds in a circle in a stationary Zeno frame but I doubt the exponential increase would be possible even with accelerating racers.

If you think it is only the clocks, an arbitrary coordinate choice, then you are talking about a mechanism to accomplish this radical increase in rate in actual physical clocks correct?

Quote by Austin0

But this seems to me to mean that finite proper time on Achilles clock could not possibly mean infinite time on a mechanically calibrated actual physical clock. SO the analogy is completely non-applicable.

Or do you still disagree?

DaleSpam said:
I still disagree, the analogy is very close, but I don't understand your most recent objection.
Any closer?
 
  • #442


DaleSpam said:
You are correct, it is not the same as the SC metric. The Zeno coordinates are defined on a flat spacetime, so there will always be some difference there. It is an analogy, not a derivation.

OK, thanks for pointing out my mistake. Unfortunately, it is too late to go and edit the post, so I hope anyone who refers to it in the future notices this update. Anyway, from post 393 we have:
\frac{dn}{dt}=\frac{v}{(100-vt) ln(2)}
and
t=\frac{100}{v}(1-2^{-n})

Substituting the second equation in on the rhs of the first equation and simplifying we get
\frac{dn}{dt}=\frac{2^n v}{100 ln(2)}

So the metric in post 414 should be:
ds^2=-c^2 \left( \frac{100 ln(2)}{2^n v} \right)^2 dn^2 + dx^2 + dy^2 + dz^2

Which again is clearly not the Minkowski metric of an inertial frame, thereby demonstrating that the Zeno coordinates are non-inertial.

Well you still have that v in the rhs of your equation. What does it represent??
The only definition of v actually expressed is in the Achilles frame so that does not seem like it could be that ,right?
So how do you define v in the Zeno frame and what does it apply too?

******************************_____
DaleSpam said:
Consider the inertial frame where Achilles is at rest. In this frame the turtle's worldline is given by (t,100-vt) where v is the relative velocity between Achilles and the turtle. So in this frame Achilles is a distance d=100-vt behind the turtle. The definition of Zeno time, n, given is d=100/2^n. Substituting in and simplifying we get the following transform between the inertial frame and Zeno coordinates:
n=log_2 \left( \frac{100}{100-vt} \right)

Taking the derivative of Zeno coordinate time wrt Achilles proper time we get
\frac{dn}{dt}=\frac{v}{(100-vt) ln(2)} \neq 1
So Achilles' clock does not run at the same rate as Zeno coordinate time.

Taking the inverse transform we get
t=\frac{100}{v}(1-2^{-n})
so
\lim_{n\to \infty } \, t = \frac{100}{v}
So as Zeno coordinate time goes to infinity Achilles proper time does not.

So in this frame Achilles is a distance d=100-vt behind the turtle. The definition of Zeno time, n, given is d=100/2^n.

You have stated that although Achilles and the tortoise are inertial, the Zeno frame is not, so how do you arrive at your identity here to justify your substitution and simplification. The d here in Achilles frame; d=100-vt is not equivalent to the d' here in Zeno's frame; d'=100/2^n. is it?
Having invoked relativistic principles in this classic scenario how can you now directly equate a distance in one frame with that in another which is not only moving at a relative velocity but which is in non-uniform motion?
What about simultaneity?
So how can the rest of your derivation from that point be valid if this initial step is not on ??
 
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  • #443


Austin0 said:
Well you still have that v in the rhs of your equation. What does it represent??

It doesn't represent anything--it's just a number that is used to describe the relationship between two coordinate systems, and also happens to be the speed of Achilles in one of the coordinate systems.

I think that you are having trouble grasping the idea of an arbitrary, noninertial, curvilinear coordinate system (as opposed to an inertial, Cartesian coordinate system). An inertial Cartesian coordinate system is set up in some standard way (for example, using light signals to measure distances and using a standard clock to measure time, and using the Einstein synchronization convention for synchronizing distant clocks). But you can use any convention you like to set up a coordinate system. Let (x,t) be an inertial Cartesian coordinate system for some region R of spacetime. Let T'(x,t), X'(x,t), X(x',t'), T(x',t') be any four differentiable functions such that for any pair (x,t) describing a point in R,

X(X'(x,t), T'(x,t)) = x
T(X'(x,t), T'(x,t)) = t

Then within region R, you can use coordinates x', t' defined by

x' = X'(x,t)
t' = T'(x,t)

As far as GR is concerned, (x',t') can be used just as well as (x,t).

In the case DaleSpam is talking about,

X'(x,t) = x
T'(x,t) = log_2(\dfrac{100}{100-vt})

You are asking what the physical interpretation of the noninertial coordinates are--coordinates don't HAVE a physical interpretation, or they don't need to, anyway. They're just a way of identifying points in spacetime. They're just names, but names chosen in a "smooth" way, so that you know that nearby points will have names that are close together as numbers.
 
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  • #444


Austin0 said:
Pervect has here given a series of events. Or at least relationships as there seems to be no determinable velocities or explicit spatial coordinates to be derived from this information.
I assumed that the distance to the Tortoise was the spatial coordinate for Achilles, but it is true that we never actually introduced a method to assign spatial coordinates elsewhere. That would require the introduction of a simultaneity convention and a spatial metric elsewhere. It could be done, but would require some more work.

However, since the only thing of interest in the scenario is Achilles I don't see the need. If you want to do more complicated scenarios which are still analogous to the SC horizon then I would recommend going to Rindler coordinates. There the analogy is even closer.

Austin0 said:
SO we have these times and relative distances and the premise that both Achilles and the tortoise are inertial with which to synthesize a coordinate system and metric.

You have asserted that the Zeno frame is non-inertial so the question is what possible state of motion of that frame could make possible those observed distances between two bodies in uniform motion.
For coordinates non-inertial just means that the metric is not the Minkowski metric, as demonstrated. There is no requirement that a coordinate system correspond with some observer's state of motion.

Austin0 said:
If the observations in the Zeno frame supported a picture of linear decrease in distance between Achilles and the tortoise this would indicate a constant motion of the Zeno frame also , agreed?
Constant motion relative to Achilles, yes. In other words, the coordinate acceleration of Achilles would be 0.

Austin0 said:
If the observed decrease in distance, itself increased in rate , this would support a conclusion of positive parallel acceleration of the Zeno frame.I.e. Zeno frame increasing it's velocity relative to A and the tortoise.

But according to Pervect the decrease in relative distance between Achilles and the tortoise is decreasing over time non-linearly.
SO what possible motion (acceleration) of the Zeno frame could make this possible?
I am not sure, but it sounds like you want the coordinate acceleration of Achilles, which is easy enough to solve. From post 393 we already found that Achilles' worldline in the Zeno coordinates is given by d = 100 \; 2^{-n}, so Achilles' coordinate acceleration is the second derivative wrt n which is a = 100 \, 2^{-n} ln(2)^2.

If this is not what you had intended, then could you be more explicit about what you want calculated?

Austin0 said:
My conclusion is that there is no possible acceleration that could do this alone and therefore the observations in the Zeno frame could only be possible if the Zeno time rate was increasing at a rate not possible through the effects of motion ( Lorentz effects..)
I agree, the same thing happens in SC. The SC coordinate time is increasing at a rate which is not possible through the effects of motion for any local observer. It is only by the use of a simultaneity convention and a distant observer that SC time is related to any observer's proper time. We haven't defined either of those for Zeno coordinates, but we certainly could do so.

Austin0 said:
Put simply:
Achilles is passing a stream of Zeno clocks and observers. Do you think Achilles sees everything in the Zeno frame speed up exponentially or only the clocks?
Only the coordinate time speeds up exponentially, physical clocks do not. Similarly with a free faller passing a stream of shell observers in SC.

Austin0 said:
If you think it is only the clocks, an arbitrary coordinate choice, then you are talking about a mechanism to accomplish this radical increase in rate in actual physical clocks correct?
Clocks measure proper time, not coordinate time. There is no mechanism for coordinates. Coordinates are a mathematical mapping from events in the manifold to R4. They are not physical. That is the whole point.
 
  • #445


Austin0 said:
Well you still have that v in the rhs of your equation. What does it represent??
As stevendaryl mentioned, it is just a parameter for the metric. Like M in the Schwarzschild metric. In fact, this is an unintentional similarity.

Austin0 said:
So in this frame Achilles is a distance d=100-vt behind the turtle. The definition of Zeno time, n, given is d=100/2^n.

You have stated that although Achilles and the tortoise are inertial, the Zeno frame is not, so how do you arrive at your identity here to justify your substitution and simplification. The d here in Achilles frame; d=100-vt is not equivalent to the d' here in Zeno's frame; d'=100/2^n. is it?
Yes, it is the same. Pervect only transformed the time coordinate.

Austin0 said:
Having invoked relativistic principles in this classic scenario how can you now directly equate a distance in one frame with that in another which is not only moving at a relative velocity but which is in non-uniform motion?
It isn't a distance, it is a coordinate. Coordinates and distances are not the same thing. In this case, the coordinate is numerically equal to a distance in an inertial frame, but it is still a coordinate not a distance.

You made similar comments about time and clocks in your previous post. Perhaps this is the root of your problem. In GR time coordinates are not readings on some clock and spatial coordinates are not measurements on some rod. They are mathematical functions which map open subsets of events in spacetime to open subsets of points in R4. They have some mathematical restrictions like being smooth, continuous, and one-to-one, but no physical restrictions. The connection to physical measurements, like clocks and rods, is done through the metric.

Austin0 said:
What about simultaneity?
You are correct, I have not defined a simultaneity convention nor any coordinates off of Achilles' worldline. However, since we are only interested in events on Achilles' worldline it is hard to see why it would matter. If you like, the easiest thing will be to take the standard simultaneity convention of Achilles' inertial frame, however that will make the analogy a bit less direct since Achilles is anlogous to a free-falling local observer and the SC simultaneity convention does not correspond to the standard simultaneity convention of a free-falling local observer.

You could make some remote non-inertial observer and give a simultaneity convention that maps his coordinates to Zeno time. This would make the analogy better, but it seems like a lot of effort.
 
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  • #446


I just read through this whole thread and it seems that it's all about relativity of simultaneity.

In the infaller's reference frame is his passage through the horizon simultaneous with some finite well defined event at the distant observer's ship (like when the distant observer is muttering to himself: "Well, it's been 2 hours since his jump, let's go home").

While the distant observer, if using Schwarzschild coordinates, does not connect these 2 events as simultaneous. In SC the infaller's passege through EH is in infinite future for the distant observer, but this distant observer can use different coordinates where the infaller's passage through EH lies in finite future. He has the choice of different coordinates because in curved spacetime the simultaneity convention is not given unambiguously.

Is it that simple, or I'm missing something?
 
  • #447


mpv_plate said:
I just read through this whole thread
That is impressive! It's a big thread.

mpv_plate said:
Is it that simple, or I'm missing something?
Yes, it is that simple. Thanks for the excellent summary.
 
  • #448


mpv_plate said:
I just read through this whole thread and it seems that it's all about relativity of simultaneity.

In the infaller's reference frame is his passage through the horizon simultaneous with some finite well defined event at the distant observer's ship (like when the distant observer is muttering to himself: "Well, it's been 2 hours since his jump, let's go home").

While the distant observer, if using Schwarzschild coordinates, does not connect these 2 events as simultaneous. In SC the infaller's passege through EH is in infinite future for the distant observer, but this distant observer can use different coordinates where the infaller's passage through EH lies in finite future. He has the choice of different coordinates because in curved spacetime the simultaneity convention is not given unambiguously.

Is it that simple, or I'm missing something?
I have yet to catch up with the last two weeks, but yes there is more - for relativity of simultaneity as in SR is quite innocent compared with "will it really happen or not". And if I now correctly understand this matter then the answer to that question (and thus also to the question of this thread) is not accessible to us. This was also somewhat discussed in https://www.physicsforums.com/showthread.php?t=656240.

It appears that some people (e.g Austin and Dalespam) are still trying to argue about this matter in this thread; I wish them good luck as to me there doesn't seem to be a possible way of deciding who is right based on logic.
 
  • #449


harrylin said:
It appears that some people (e.g Austin and Dalespam) are still trying to argue about this matter in this thread; I wish them good luck as to me there doesn't seem to be a possible way of deciding who is right based on logic.
I am not sure which specific topic you are referring to by "this matter", but the whole point of expressing a physical theory in terms of a mathematical framework is precisely in order to ensure that the conclusions/predictions follow logically from the premises/postulates. You just seem to have difficulty with the mathematical framework which enforces the logic. That is a natural part of learning a challenging topic, but it does not in any way indicate a deficit in the logic of the theory.
 
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  • #450


Quote by Austin0

Well you still have that v in the rhs of your equation. What does it represent??

stevendaryl;4215692 1) said:
It doesn't represent anything--2) it's just a number that is used to describe3) the relationship between two coordinate systems, and also happens to be 4) the speed of Achilles in one of the coordinate systems. .

Well i asked a perfectly cogent and relevant question. 1)you deny it is a valid question . then 2) you immediately contradict yourself and present two different possible reasonable answers 3),and 4) but both your answers seem questionable.

Working from the information defined by pervect it is not possible to derive a velocity for the Achilles frame in the Zeno frame as far as i can see,
Likewise it is not possible to define a velocity for Achilles himself in the Zeno frame.
So again I ask what is the velocity referring to that could be a valid part of the Zeno metric?.
And how do you arrive at it??

stevendaryl said:
I think that you are having trouble grasping the idea of an arbitrary, noninertial, curvilinear coordinate system (as opposed to an inertial, Cartesian coordinate system).

I have no trouble with the idea of an arbitrary non-linear coordinate system.
In fact, back at my second post I brought up this possibility

Quote by Austin0
Having done so it appears that it was not explicitly stated that the intervals were equivalent. And in fact they would not correspond to time on any normal clock with a constant rate.
So are you talking about an arbitrary clock that speeds up over time ??

DaleSpam denied this back then but it appears that that is exactly the case here,,,, DO you now agree??

stevendaryl said:
An inertial Cartesian coordinate system is set up in some standard way (for example, using light signals to measure distances and using a standard clock to measure time, and using the Einstein synchronization convention for synchronizing distant clocks). But you can use any convention you like to set up a coordinate system. Let be an inertial Cartesian coordinate system for some region of spacetime.
Let (x,t) be an inertial Cartesian coordinate system for some region R of spacetime. Let T'(x,t), X'(x,t), X(x',t'), T(x',t') be any four differentiable functions such that for any pair (x,t) describing a point in R,

X(X'(x,t), T'(x,t)) = x
T(X'(x,t), T'(x,t)) = t

Then within region R, you can use coordinates x', t' defined by

x' = X'(x,t)
t' = T'(x,t)

As far as GR is concerned, (x',t') can be used just as well as (x,t).
this appears to me to be a generalization of the concept of transformation between relative frames. Is this correct??
if this is so i don't see the relevance.
This particular case is not about setting up a system from the ground but working within the constraints of defined relationships and partial definitions without a completely defined system for Zeno .We can assume a standard inertial system for Achilles but we have only some data from observations in Zeno frame to go by.

DaleSpam said:
Consider the inertial frame where Achilles is at rest. In this frame the turtle's worldline is given by (t,100-vt) where v is the relative velocity between Achilles and the turtle. So in this frame Achilles is a distance d=100-vt behind the turtle. The definition of Zeno time, n, given is d=100/2^n. Substituting in and simplifying we get the following transform between the inertial frame and Zeno coordinates:
n=log_2 \left( \frac{100}{100-vt} \right)

Don't you agree that to assert an equivalence between coordinates or values between two frames in relative motion you need to transform the values from one frame to the other.
If in fact you do not already have the correct transform functions, the T,X,T' and X' in your generalization you cannot simply assume the equivalence between some values in both frames and derive a valid transform from that . There has to be some relevant basis for the equivalence from first principles to justify such an identity and substitution.
Wouldn't you agree??
SO in this case we are given : d=100-vt in the A frame and d=100/2^n in the Z frame.

Is the 100 in the A frame equivalent to the 100 in the Z frame?
Assuming that at A time t =0 Achilles is at x=0 and the tortoise is at x=100 and at Z time n= 0 Achilles is at x'=0 and the tortoise is at x'=100. isn't it axiomatic that if these events are simultaneous in the A frame that they cannot be simultaneous in the Z frame?? It follows that the distances , the spatial intervals in the two frames cannot be congruent also Yes??
So if the intervals dx,t=0 and dx', t'=0 are not equivalent, even initially when you can assign coordinates to the positions in the Z frame, how do you justify the equivalence 100-vt=100/2^n over time when the systems are not only in relative motion but one of them is non-linear??

Where you do not have a basis to even determine coordinate positions in the Z frame for A and the tortoise or relate times in that frame to the A frame??

It appears to me that to make this assumption of equivalence is unfounded and circular. I.e.,,to determine if these are equivalent requires a valid transformation so to use them to derive a transformation then makes them equivalent circularly.

stevendaryl said:
In the case DaleSpam is talking about,

X'(x,t) = x
T'(x,t) = log_2(\dfrac{100}{100-vt})

stevendaryl said:
You are asking what the physical interpretation of the noninertial coordinates are--coordinates don't HAVE a physical interpretation, or they don't need to, anyway. They're just a way of identifying points in spacetime. They're just names, but names chosen in a "smooth" way, so that you know that nearby points will have names that are close together as numbers. .

in another thread you stated that gravitational time dilation could be eliminated by a coordinate choice remember??
I asked you if you were talking about an arbitrary scaling of clock periodicity and you agreed, correct?
So then we are talking about a physical interpretation of clock rates. AN artificial mechanical adjustment to the workings of the mechanism. What could be clearer than that??
In this case this means a mechanistic device that exponentially increases the rate at which the hands spin or the LED increments or whatever means that is used to actually indicate the measure of time,,,, CORRECT?
Such artificial scaling is in fact used in the GPS system right?? Those clocks physically increment at a different rate yes??
 
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