Which Train Explodes First in the Time Dilation Paradox?

  • #51
ghwellsjr said:
I think this could be misleading. "Events" in SR jargon have a wider meaning than merely when something significant "happens" in a scenario. [..]whether or not anything is present at that location and at that time [..]
Such extreme jargon would loose all connection to the true meaning of the word.
IMHO the following summarizes "event" rather well:
http:http://en.wikipedia.org/wiki/Event_(relativity)
 
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  • #52
altergnostic said:
I meant to say that ANY two frames may disagree on observatios, not the two specified in this particular problem. I was generalising, i guess this wasnt clear. If you have three frames with different relative velocites to each other they will not agree on the time of their observatios on events occurring on all three of them.
I'm not sure you have a clear understanding here, but even if you do, you are not expressing it clearly. Any two frames will always agree on "observations" if by that we mean what observers will observe. What they will not agree on is their assignment of the coordinate values of events. There is clear terminology to express what you seem to be saying, why not use it? Instead of saying:
If you have three frames with different relative velocites to each other they will not agree on the time of their observatios on events occurring on all three of them.
Why not say:
If you have three frames with different relative velocities to each other they will not agree on the coordinate times of the events occurring on all three of them.

altergnostic said:
If light from a source takes longer to reach an observer than another, they will not agree. They will agree on observations when the situation is symmetrical.
It's statement like this that makes me wonder if you really understand SR. What is it that you are saying they don't agree on or do agree on? Observations? If you are saying that two distant observers will see the same thing at the same time if they are the same distance from the source of the observation, then that really begs the question. How do you know that they are the same distance and that their observations are taken at the same time? That's an issue that requires a frame to settle, not observations.

Or are you saying that they will agree on the coordinate location and time of a remote event? Well this will be true if they are both using the same frame and they are both discussing the same event.

Look, in this scenario, when we are talking about the symmetry of observations, we are not talking about either of these things. We are saying that each observer sees the other ones clock ticking slower than his own by the same ratio and this is independent of any frame and it is not an observation of time dilation. Note that the observers are not observing the same events, the first observer is observing the second observer's clock in relation to his own and the second observer is observing the first observer's clock in relation to his own.
altergnostic said:
bgq said:
Each of the observers in the train "observes" that the clock of the other is slower. Observer in train A observes that clock of B is slower than clock of A, but observer in train B observes that clock of A is slower than that of B. There is a clear disagreement about what each observes.
That's a calculation, not an observation. The observation is "light signal at t seconds on my watch" and from there you calculate the difference between clocks. Remember, observations are local events, light has to reach you, be inside your own frame, you can't see light at a distance. Everything that happens on another frame at a considerable distance and/or relative velocity has to be calculated.
Again, even if you understand SR correctly, you're not expressing it correctly. You seem to be incorporating more than one frame to explain what is happening. Stick with one frame at a time. And I'm not sure when you say that bgq's statement is regarding a calculation rather than an observation is correct. His statement about their observations is correct. His statement that there is disagreement is not correct. I don't know what you mean by:
The observation is "light signal at t seconds on my watch" and from there you calculate the difference between clocks.
What calculation in the difference between the clocks are you talking about?

You are correct that observations are local events because light has to reach you, but why do you say "inside your own frame" and why do you say "on another frame at a considerable distance"? In SR, all inertial frames cover all distances. It's not like I'm in one frame local in extent to me and the other observer, who is at a considerable distance away from me (whether or not he is moving with respect to me) is in another frame local in extent to him. If you want to consider my rest frame, then it also includes that distant other observer. Or if you want to consider his rest frame, then it also includes me. In my rest frame, my clock ticks at the same rate as the coordinate time and his moving clock ticks at a slower rate. In his rest frame, his clock ticks at the same rate as the coordinate time and my clock ticks slower. In a frame in which we are both traveling at the same speed, both our clocks tick slower, by the same amount, than the coordinate time.
 
  • #53
harrylin said:
Such extreme jargon would loose all connection to the true meaning of the word.
IMHO the following summarizes "event" rather well:
http:http://en.wikipedia.org/wiki/Event_(relativity)
There are multiple "true meanings" of the word "event". The wikipedia article is pointing out that "a glass breaking on the floor" is not the idealized event that we use in SR which does not have an extent either in space or in time. To call the idealized meaning of the word "event" when applied to the Lorentz Transformation process as extreme jargon is to discredit an understanding what I was trying to point out. "Event" has a very specific meaning in Special Relativity that many people are confused about specifically because they want to link it to a happening such as a concert which is also called an event.
 
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  • #54
ghwellsjr said:
[..] To call the idealized meaning of the word "event" when applied to the Lorentz Transformation process as extreme jargon is to discredit an understanding what I was trying to point out.[..]
I find the idealized meaning of the word "event" as currently described in Wikipedia acceptable jargon, in contrast with your description which I called extreme jargon. Thus we don't appreciate each other's explanations of this; and that is no problem, as everyone can verify the references and make up his/her own mind while taking the best of both. :smile:
 
  • #55
ghwellsjr said:
Consider a new situation where two observers are approaching each other from a great distance apart. They will each observe the other ones clock as running faster than their own
.
Actually, I don't understand why each observes the other clock faster, the time dilation formula does say nothing about the direction of motion, can you clarify this to me?
 
  • #56
harrylin said:
I find the idealized meaning of the word "event" as currently described in Wikipedia acceptable jargon, in contrast with your description which I called extreme jargon. Thus we don't appreciate each other's explanations of this; and that is no problem, as everyone can verify the references and make up his/her own mind while taking the best of both. :smile:
Then are you saying that if I specify a set of coordinates in a particular frame, say at t=3 seconds, x=4, y=5 and z=6 (all in light-seconds) but there is nothing but empty space at that location at that time, then it is not an event?
 
  • #57
bgq said:
Actually, I don't understand why each observes the other clock faster, the time dilation formula does say nothing about the direction of motion, can you clarify this to me?
I've been trying to say that you can't observe time dilation, it's a calculation based on the speed in an arbitrarily selected inertial frame of reference. If you could observe it, it would be a bunch of different values depending on which frame someone chooses. An observation is what you actually see with your eyes or with an instrument like a telescope or a radio or a television. These all depend on the changing light travel time which makes things appear faster when approaching or slower when receding. Doppler is what you observe, time dilation is what you calculate.
 
  • #58
ghwellsjr said:
I've been trying to say that you can't observe time dilation, it's a calculation based on the speed in an arbitrarily selected inertial frame of reference. If you could observe it, it would be a bunch of different values depending on which frame someone chooses. An observation is what you actually see with your eyes or with an instrument like a telescope or a radio or a television. These all depend on the changing light travel time which makes things appear faster when approaching or slower when receding. Doppler is what you observe, time dilation is what you calculate.

Well, I think I had a problem with the exact meaning of "observation" which lead to some confusion; anyway I think I now get it.
Thanks.
 
  • #59
I'll add what I hope is the simplest possible separation of measurement versus assignment (of coordinates or labels).

Bob and Alice, each with a wristwatch, have relative motion and pass each other. We don't care about anything except the event they go right past each other.

There are two measurements here: Bob reads his watch at passage and see 2 PM. Alice read her watch and sees 3 PM. Each can see the other's watch, so Bob agrees that Alice measured 3 PM. Alice agrees that Bob measured 2 PM. Everyone in universe who can gain information about these measurements agrees on the result of each of these two measurements.

What differs by frame or observer is the time assigned to the passing event. Bob assigns 2 PM to the event. Alice assigns 3 PM to the event. Other observers will assign different time to this same 'passing' event.
 
  • #60
PAllen said:
I'll add what I hope is the simplest possible separation of measurement versus assignment (of coordinates or labels).

Bob and Alice, each with a wristwatch, have relative motion and pass each other. We don't care about anything except the event they go right past each other.

There are two measurements here: Bob reads his watch at passage and see 2 PM. Alice read her watch and sees 3 PM. Each can see the other's watch, so Bob agrees that Alice measured 3 PM. Alice agrees that Bob measured 2 PM. Everyone in universe who can gain information about these measurements agrees on the result of each of these two measurements.

What differs by frame or observer is the time assigned to the passing event. Bob assigns 2 PM to the event. Alice assigns 3 PM to the event. Other observers will assign different time to this same 'passing' event.

OK, that's clear.
 
  • #61
PAllen said:
I'll add what I hope is the simplest possible separation of measurement versus assignment (of coordinates or labels).

Bob and Alice, each with a wristwatch, have relative motion and pass each other. We don't care about anything except the event they go right past each other.

There are two measurements here: Bob reads his watch at passage and see 2 PM. Alice read her watch and sees 3 PM. Each can see the other's watch, so Bob agrees that Alice measured 3 PM. Alice agrees that Bob measured 2 PM. Everyone in universe who can gain information about these measurements agrees on the result of each of these two measurements.

What differs by frame or observer is the time assigned to the passing event. Bob assigns 2 PM to the event. Alice assigns 3 PM to the event. Other observers will assign different time to this same 'passing' event.
This can even be confusing because you are implying that just because Bob and Alice have their own watches (which always keep Proper Time) that they will automatically use that for the coordinate time of their own rest frames which is not a requirement specifically if they are not inertial. Furthermore, it is convenient to use the Standard Configuration for assigning Coordinate times and locations, otherwise, you cannot use the simple version of the Lorentz Transform to convert coordinates from one frame to another. When you do that, it would be most convenient to assign the origins of their two rest frames to the event of their passing and then calculate their Proper Times as an offset from those (along with whatever time dilation is required). The way you are doing it requires an awful lot of complicated computation to convert events from one frame to the other. Why can't we capitalize on the conventional easy way of doing and expressing these things, especially to novices? Once they grasp the simple way to understand Special Relativity, they can go off into all the other complicated ways that don't add one single thing to the understanding of SR.
 
  • #62
ghwellsjr said:
This can even be confusing because you are implying that just because Bob and Alice have their own watches (which always keep Proper Time) that they will automatically use that for the coordinate time of their own rest frames which is not a requirement specifically if they are not inertial. Furthermore, it is convenient to use the Standard Configuration for assigning Coordinate times and locations, otherwise, you cannot use the simple version of the Lorentz Transform to convert coordinates from one frame to another. When you do that, it would be most convenient to assign the origins of their two rest frames to the event of their passing and then calculate their Proper Times as an offset from those (along with whatever time dilation is required). The way you are doing it requires an awful lot of complicated computation to convert events from one frame to the other. Why can't we capitalize on the conventional easy way of doing and expressing these things, especially to novices? Once they grasp the simple way to understand Special Relativity, they can go off into all the other complicated ways that don't add one single thing to the understanding of SR.

I wanted to bypass the issues of setting up a complete coordinate system, and transforming between them, to focus exclusively, in isolation, on the distinction between measurement and assigning a single coordinate label in one obvious way. I feel reducing to this simplest case is helpful. Sorry if you don't.
 
  • #63
PAllen said:
I wanted to bypass the issues of setting up a complete coordinate system, and transforming between them, to focus exclusively, in isolation, on the distinction between measurement and assigning a single coordinate label in one obvious way. I feel reducing to this simplest case is helpful. Sorry if you don't.
But how does your example show the distinction between the measurement of Proper Time on a watch and the assigning of Coordinate Time when they are the same for each observer?

You say other observers will assign different times to this same 'passing' event but wouldn't they also have to be present at the same 'passing' event if your simplest case is how they assign Coordinate Time based on the arbitrary Proper Time displayed on their watches?
 
  • #64
ghwellsjr said:
But how does your example show the distinction between the measurement of Proper Time on a watch and the assigning of Coordinate Time when they are the same for each observer?

You say other observers will assign different times to this same 'passing' event but wouldn't they also have to be present at the same 'passing' event if your simplest case is how they assign Coordinate Time based on the arbitrary Proper Time displayed on their watches?

I am not bothering to make such distinctions, or get into details of how other observers might assign a time (just that they could, and wouldn't generally pick the same values), or that Bob and Alice have other choices besides the obvious one. I am focusing purely on the distinction between measurements and the act of choosing a coordinate value.

I believe there was confusion on this specific point, and I wanted to focus on it in isolation. I believe it was helpful.

I do not want to belabor this anymore.
 
  • #65
ghwellsjr said:
Then are you saying that if I specify a set of coordinates in a particular frame, say at t=3 seconds, x=4, y=5 and z=6 (all in light-seconds) but there is nothing but empty space at that location at that time, then it is not an event?
For me that's just a space-time coordinate. Regretfully the Wikipedia article only paraphrases the referenced textbooks, so here's a citation of how Alonso and Finn (Fundamental University Physics) define "event" in their chapter on the Lorentz transformation:

"An event is a specific occurrence that happens at a particular point in space and at a particular time".

I won't comment further on this except if it's an issue for bgq.
 
  • #66
ghwellsjr said:
I'm not sure you have a clear understanding here, but even if you do, you are not expressing it clearly. Any two frames will always agree on "observations" if by that we mean what observers will observe. What they will not agree on is their assignment of the coordinate values of events. There is clear terminology to express what you seem to be saying, why not use it?
It's statement like this that makes me wonder if you really understand SR. What is it that you are saying they don't agree on or do agree on? Observations?

Yes, i meant the coordinates in space and time, not what they see. I didn't speak of coordinates of events since it was clear, i think, we were always talking about coordinates, not if one sees an explosion and the other sees jerry seinfeld, but ok, there's better terminology indeed.

ghwellsjr said:
What calculation in the difference between the clocks are you talking about?

When you compare the rate of two clocks you are already calculating. You are computing the difference between the time in your clock and the observed time on a clock located in the primed frame, that's all. You will se a prevously sync'd clock going slower.

ghwellsjr said:
You are correct that observations are local events because light has to reach you, but why do you say "inside your own frame" and why do you say "on another frame at a considerable distance"? In SR, all inertial frames cover all distances. It's not like I'm in one frame local in extent to me and the other observer, who is at a considerable distance away from me (whether or not he is moving with respect to me) is in another frame local in extent to him. If you want to consider my rest frame, then it also includes that distant other observer. Or if you want to consider his rest frame, then it also includes me. In my rest frame, my clock ticks at the same rate as the coordinate time and his moving clock ticks at a slower rate. In his rest frame, his clock ticks at the same rate as the coordinate time and my clock ticks slower. In a frame in which we are both traveling at the same speed, both our clocks tick slower, by the same amount, than the coordinate time.

I say that it is in your own frame because seeing light is always a local event, you can't speak of light in another frame. I mean that regardless of the position and motion of another frame, light is either in your own frame right in your eyes, or you are not aware of it at all. And i said "considerable distance" because at small distances / velocities we don't really need to consider special relativity. And another frame is the primed frame, not a frame that is no longer inside your own frame, just a frame that would locally measure its own coordinates to be in disagreement with your observations. If i see my clock at 2s and yours at 1s, you would see your own at 2s and mine at 1s. Yours at 1 and yours at 2 are different measurements, that's what "separetes" frames.
Now, when you talk of a frame in which we are both traveling at the same speed you are talking about a third frame, right? If so, i agree with all you have said.
 
  • #67
altergnostic said:
I say that it is in your own frame because seeing light is always a local event
Seeing light is local, but frames are not local. So this is a reason to not use your terminology.
 
  • #68
DaleSpam said:
Seeing light is local, but frames are not local. So this is a reason to not use your terminology.

But seeing light is always done in your own frame, i don't see any problem with it other than being redundant.
 
  • #69
altergnostic said:
But seeing light is always done in your own frame
No, this is incorrect. If I see the light in one frame then I see it in all frames. Changing coordinate systems does not make me blind as you suggest. I do not need to use any particular coordinate system in order to see.
 
  • #70
altergnostic said:
But seeing light is always done in your own frame, i don't see any problem with it other than being redundant.

"Your frame" is another of those dangerous phrases that can lead to misunderstanding. It is a convenient shorthand for "the frame in which you just coincidentally happen to have zero instantaneous velocity" - and if you try substituting that for the bolded text you may see the problem with saying that you do anything (including seeing) "in a frame".

Events, such as light hitting your retina, don't happen in frames. They just happen; and different frames are just different sets of rules for assigning them space and time coordinates.
 
  • #71
Nugatory said:
"Your frame" is another of those dangerous phrases that can lead to misunderstanding. It is a convenient shorthand for "the frame in which you just coincidentally happen to have zero instantaneous velocity" - and if you try substituting that for the bolded text you may see the problem with saying that you do anything (including seeing) "in a frame".

Events, such as light hitting your retina, don't happen in frames. They just happen; and different frames are just different sets of rules for assigning them space and time coordinates.

Well, I meant to point out that light seen by one observer will not be seen by another, even if the photons are radiated from the same event, each observer sees a different set of photons, and each observer draws his own coordinates (which may or may not coincide with someone else's coordinates), hence, the same light is seen in only one frame of reference, even if it exists in every frame. I guess i should've just said observer instead of frame and save us all from this waste of time.
 
  • #72
altergnostic said:
[..] I guess i should've just said observer instead of frame and save us all from this waste of time.
That's better, since anyone can freely choose whatever frame he wants. However it's not really a waste of time, as wrong ways of saying things can propagate misunderstanding.
 
  • #73
altergnostic said:
[..] I say that it is in your own frame because seeing light is always a local event, you can't speak of light in another frame. I mean that regardless of the position and motion of another frame, light is either [..] right in your eyes, or you are not aware of it at all. [..].
altergnostic said:
Well, I meant to point out that light seen by one observer will not be seen by another, even if the photons are radiated from the same event, each observer sees a different set of photons, and each observer draws his own coordinates [..]
In addition to my earlier post of today, this may serve as illustration. Even after eliminating the frame/observer mix-up, you seem to suggest that we can explain SR by using QM (photons), so that an observation by one observer cannot be matched by another observer. If so, then that completely misses the point. SR is based on Maxwell's wave mechanics and shows how the same light wave and even the same phase difference (which can in principle be detected with different detectors) is mapped differently with different reference systems.
Compare the train and station example: one light flash as detected with different reference systems
- http://www.bartleby.com/173/9.html
 
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  • #74
i think my brain is going to melt.

everyone has deviated from the original problem. how can person A survive while person B explodes, and vice versa?
 
  • #75
holtto said:
[..] everyone has deviated from the original problem. how can person A survive while person B explodes, and vice versa?
- The problem of the OP was already answered with posts #2, 4, 5 etc.
- Very detailed answers can be found in posts #17, #21.
- References to similar problems and discussions can be found in post #33.

What followed was just a little "after talk". :smile:
 
  • #76
harrylin said:
- The problem of the OP was already answered with posts #2, 4, 5 etc.
- Very detailed answers can be found in posts #17, #21.
- References to similar problems and discussions can be found in post #33.

What followed was just a little "after talk". :smile:
hmmm, only #5 and #21 seem to have some concrete stuff; too bad they had been buried under all the "after talk."I like this paradox, let's call it the "Action Movie Train Scene" paradox.
 
  • #77
so let me guess this straight. the resolution is:

In Adam's frame, Bob dies before Adam dies

In Bob's frame, Adam dies before Bob dies.

In the end, both of them die. Everybody dies.
 
  • #78
holtto said:
so let me guess this straight. the resolution is:

In Adam's [rest] frame, Bob dies before Adam dies

In Bob's [rest] frame, Adam dies before Bob dies.

In the end, both of them die. Everybody dies.
[EDITED] Indeed both of them die (and I added a little precision in [], as explained in post #70).
However - as also illustrated in post #21 - the local clocks must show the same time when they blow up; and as according to each frame's reckoning the distant clock appears to run slower (with synchronous start), this means that "In Adam's [rest] frame, Bob dies after Adam dies."

Anyway, neither of them can see the destruction of the other train. You could put "In the end, both of them die; and neither saw the other die".

PS: The easiest frame to pick is the rest frame of the train station. Using that frame, the symmetry of the situation remains clear and it immediately shows that each train starts exploding before information of the other train's explosion can reach it.
 
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  • #79
altergnostic said:
Well, I meant to point out that light seen by one observer will not be seen by another, even if the photons are radiated from the same event, each observer sees a different set of photons
This is all true, it just has nothing to do with reference frames.

altergnostic said:
and each observer draws his own coordinates (which may or may not coincide with someone else's coordinates), hence, the same light is seen in only one frame of reference, even if it exists in every frame.
Suppose that you have a detector on the optic nerve. If the observer sees the light then the detector prints out a piece of paper with the number 1, if the observer does not see the light then the detector prints out a piece of paper with the number 0. If the observer sees the light in one frame of reference there is a 1 on the piece of paper. You are claiming that in some frames there will be a 0 on the piece of paper. That is wrong.

altergnostic said:
I guess i should've just said observer instead of frame and save us all from this waste of time.
Yes, but it is such a common mistake that it deserves a remine
 
  • #80
DaleSpam said:
Suppose that you have a detector on the optic nerve. If the observer sees the light then the detector prints out a piece of paper with the number 1, if the observer does not see the light then the detector prints out a piece of paper with the number 0. If the observer sees the light in one frame of reference there is a 1 on the piece of paper. You are claiming that in some frames there will be a 0 on the piece of paper. That is wrong.

No, that's not what i am saying. you will se the number 1 in a paper if someone else sees a beam of light, but you will not see the beam itself. I am saying that light that gets in your retina doesn't go into anywhere else but your retina. If a photon is in your eye it is not in someone else's eye. If you know about light being seen by another observer, you do only by indirect means, like a paper with the number 1 in your example.
 
  • #81
holtto said:
so let me guess this straight. the resolution is:

In Adam's frame, Bob dies before Adam dies

In Bob's frame, Adam dies before Bob dies.

In the end, both of them die. Everybody dies.

No. In adam's frame, he dies before bob. In bob's, he is the one who dies first.

Both die, but the other is late, light from the explosion that comes from bob takes a while to get to adam, so when it reaches adam, he has already exploded, and vice versa.
 
  • #82
harrylin said:
In addition to my earlier post of today, this may serve as illustration. Even after eliminating the frame/observer mix-up, you seem to suggest that we can explain SR by using QM (photons), so that an observation by one observer cannot be matched by another observer. If so, then that completely misses the point. SR is based on Maxwell's wave mechanics and shows how the same light wave and even the same phase difference (which can in principle be detected with different detectors) is mapped differently with different reference systems.
Compare the train and station example: one light flash as detected with different reference systems
- http://www.bartleby.com/173/9.html

I'm not trying to explain relativity with photons. If you like, you can change photons for a directinalized beam, like a laser. If a blink of light propagates spherically, all observers will eventually see it, but they are not seeing the same patch of light. If i send a laser beam into your eye, you are the only one who will see it. And this has nothing to do with relativity or the topic anymore.
 
  • #83
harrylin said:
That's better, since anyone can freely choose whatever frame he wants. However it's not really a waste of time, as wrong ways of saying things can propagate misunderstanding.

In a thought problem, yes, you can pick any frame you like, but in real life, the observer is always attatched to his particular frame of reference, he can't choose freely nor change frames. Ever.
 
  • #84
altergnostic said:
No, that's not what i am saying. you will se the number 1 in a paper if someone else sees a beam of light, but you will not see the beam itself. I am saying that light that gets in your retina doesn't go into anywhere else but your retina. If a photon is in your eye it is not in someone else's eye. If you know about light being seen by another observer, you do only by indirect means, like a paper with the number 1 in your example.
None of your explanation has anything to do with frames, which is why your statement "the light is seen in only one frame of reference" was wrong. That incorrect statement implies exactly what I described above, which is clearly not what you meant, but is in fact what you said.

The correct statement is "the light is seen by only one observer", which is a true statement regardless of which coordinate system you choose to analyze it in.
 
  • #85
altergnostic said:
In a thought problem, yes, you can pick any frame you like, but in real life, the observer is always attatched to his particular frame of reference, he can't choose freely nor change frames. Ever.
Sure he can. A reference frame is a purely mental construct, a coordinate system, which is just a mathematical bookkeeping convention.

An observer is always free to use a coordinate system in which he is moving. In fact, mentally I suspect that you yourself do this whenever you are driving or playing a sport, you probably mentally use the reference frame of the road or field, even though you are moving in it.

That is all a reference frame is, a mental way to label distances and directions and speeds, you don't need to restrict yourself to one and you can freely choose and change frames for any reason or no reason at all.
 
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  • #86
harrylin said:
[..] you seem to suggest that [...], so that an observation by one observer cannot be matched by another observer. If so, then that completely misses the point. SR [..] shows how the same light wave [..] is mapped differently with different reference systems. [..]
altergnostic said:
[..] If a blink of light propagates spherically, all observers will eventually see it, but they are not seeing the same patch of light. If i send a laser beam into your eye, you are the only one who will see it. And this has nothing to do with relativity [..]
That's just what I meant... :rolleyes:
 
  • #87
harrylin said:
For me that's just a space-time coordinate. Regretfully the Wikipedia article only paraphrases the referenced textbooks, so here's a citation of how Alonso and Finn (Fundamental University Physics) define "event" in their chapter on the Lorentz transformation:

"An event is a specific occurrence that happens at a particular point in space and at a particular time".

I won't comment further on this except if it's an issue for bgq.

Also an event/ change-of-state has to generate an em signal to be perceived, otherwise it's a non event.
 
  • #88
The observer's perception corresponds to his position and his local clock. He is his own frame of reference. He can't make an observation from another frame of reference moving relative to himself or use the time of that frames clock.

The fact that 2 observers can't occupy the same spatial position at the same time, requires that their descriptions of an event differ. This was common knowledge thousands of years ago.

If a single photon is emitted, only the observer in line with its path will detect it.
No one else detects it!
If this were not true, then alignments in experiments wouldn't be necessary, and a detector could be placed anywhere in the lab.

If we carry the nit-picking to its conclusion, the 'frame' is another of those ideal concepts that cannot be realized. The first approximation is a set of objects with no relative motion, excluding thermal. In the real world, everything moves.

Remember, definitions are either in terms of other definitions, or circular.
 
  • #89
This is offered as another 'no calculation' demo.
The ops' original scenario has been transferred from trains to space cans (more realistic) with arbitrarily chosen speeds (a generalization). Each can sends a detonation signal when its clock indicates t, to the other can, which has a hidden exlosive device. The hyperbola indicates time t for each can depending on its speed. Signal A to B is path (1,2), signal B to A is path (3,4). No speeds are given because they aren't relevant. If B's speed varies from that of A toward light speed c, it will always send a signal before intercepting the A signal, since the hyperbola and path (1,2) never meet.

https://www.physicsforums.com/attachments/51449
 
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  • #90
phyti said:
The observer's perception corresponds to his position and his local clock. He is his own frame of reference. He can't make an observation from another frame of reference moving relative to himself or use the time of that frames clock.

The fact that 2 observers can't occupy the same spatial position at the same time, requires that their descriptions of an event differ. This was common knowledge thousands of years ago.

If a single photon is emitted, only the observer in line with its path will detect it.
No one else detects it!
If this were not true, then alignments in experiments wouldn't be necessary, and a detector could be placed anywhere in the lab.

If we carry the nit-picking to its conclusion, the 'frame' is another of those ideal concepts that cannot be realized. The first approximation is a set of objects with no relative motion, excluding thermal. In the real world, everything moves.

Remember, definitions are either in terms of other definitions, or circular.

That was my point a few posts back, but you articulated it way better. Your reminder that two can't occupy the same place at the same time is all we need to forbid any notion of light seen in another observer's frame. In real life, that light can never be directly a part of our data, we can only know of its existence through secondary effects, like "yeah, i saw that too!"
 
  • #91
phyti said:
The observer's perception corresponds to his position and his local clock. He is his own frame of reference. He can't make an observation from another frame of reference moving relative to himself or use the time of that frames clock.

So, if you are riding a bicycle, you are not entitled to think you are moving; you must insist that the ground is moving? [edit: and if, while riding a bike, I look at a clock tower, I must ignore its time because it is not in my frame.]

More germane to physics, for all these years of colliding particles or ions into stationary targets, physicist were acting incorrectly when they chose to record observations and do calculations in the COM frame rather than the lab frame?
 
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  • #92
altergnostic said:
Well, I meant to point out that light seen by one observer will not be seen by another. [..] I guess i should've just said observer instead of frame and save us all from this waste of time.
altergnostic said:
[..] If a blink of light propagates spherically, all observers will eventually see it, but they are not seeing the same patch of light. If i send a laser beam into your eye, you are the only one who will see it. And this has nothing to do with relativity or the topic anymore.
altergnostic said:
[..] Your reminder that two can't occupy the same place at the same time is all we need to forbid any notion of light seen in another observer's frame. In real life, that light can never be directly a part of our data, we can only know of its existence through secondary effects, like "yeah, i saw that too!"
Evidently you recognized that:
- saying "frame" for "a light detector" (or a person who observes) is a mix-up;
- and "the same patch of light" has nothing to do with relativity or this topic;

Thus it's a mystery to me why you continue introducing these things...
 
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  • #93
holtto said:
hmmm, only #5 and #21 seem to have some concrete stuff; too bad they had been buried under all the "after talk."


I like this paradox, let's call it the "Action Movie Train Scene" paradox.

I am very happy to know that you like this paradox; however, the "after talk" here is very valuable, I have learned from them much although I am not qualified enough to participate in these discussions.
 
  • #94
phyti said:
The fact that 2 observers can't occupy the same spatial position at the same time, requires that their descriptions of an event differ.
altergnostic said:
That was my point a few posts back, but you articulated it way better. Your reminder that two can't occupy the same place at the same time is all we need to forbid any notion of light seen in another observer's frame.
Welcome to the discussion phyti, you are making the same mistake that altergnostic is making. You can pat each other on the back all you want for being wrong together. The rather trivial fact that two observers cannot occupy the same place at the same time has absolutely nothing whatsoever to do with the question of which reference frames are admissible.

Their description of a given event certainly CAN use the same reference frame, despite the fact that they are in different locations and potentially moving wrt each other. If I get pulled over for going 100 mph then I am perfectly justified in saying that I was going 100 mph, I am not required to say that I was at rest and the officer was going -100 mph.

I am not required to use a reference frame where I am at rest, and I am not required to use a reference frame where I am at the origin.

phyti said:
He can't make an observation from another frame of reference moving relative to himself or use the time of that frames clock.
Yes, he can. GPS satellites do it all the time.

phyti said:
If a single photon is emitted, only the observer in line with its path will detect it.
No one else detects it!
Sure. But that observer detects that photon regardless of what coordinate system you choose to use to analyze the detection. You and altergnostic both seem to confuse the physical observer/detector and the purely mathematical construct of a coordinate system.
 
  • #95
altergnostic: #90
... Your reminder that two can't occupy the same place at the same time is all we need to forbid any notion of light seen in another observer's frame.

That would not be true if the event in common involved multiple photons. In Einsteins train scenario, both observers saw the flashes because they were multiple photon events. My statement was a logical basis for expecting different descriptions of events from 2 different observers. If 10 people circled a statue and each took a photo, each would have a different perspective as evidenced in the photos, yet they would agree there was only 1 statue. That's a simple case with no motion.

In real life, that light can never be directly a part of our data, we can only know of its existence through secondary effects, like "yeah, i saw that too!"
Not sure of what you are saying here, but we perceive the universe indirectly. Light is the messenger and via sensory input, says 'something happened over here', and indicates a direction.
From other posts:
When you discuss A and B observing each others clock running slower than their own, remember each is comparing his current clock event with a clock event in the others past. Does that have any useful meaning?
 
  • #96
PAllen #91
So, if you are riding a bicycle, you are not entitled to think you are moving; you
must insist that the ground is moving? [edit: and if, while riding a bike, I look at a
clock tower, I must ignore its time because it is not in my frame.]

If you read post 88 carefully, it doesn't imply any of what you said. It was just a
response to all the confusing 'frame' talk.
On a bike, on a park bench, it's irrelevant, because all things are moving. SR theory
just says if you are moving, you may choose to assume a pseudo rest frame, and
regardless of which you choose, you use a local clock. In your scenario, which was
not the intended range of application, there would be no significant difference in
using the bikers watch or the clock tower (assuming synchonization).With reference
to the observers frame, A.E. states in the 1905 paper, "It is essential to have time
defined by means of stationary clocks in the stationary system,"

More germane to physics, for all these years of colliding particles or ions into
stationary targets, physicist were acting incorrectly when they chose to record
observations and do calculations in the COM frame rather than the lab
frame?

That's just tranforming from one origin to another, which is what SR does. I don't
see any problem there.
 
  • #97
For those who may not have accepted the geometry based example, and motivated by ghwells example using doppler methods, this is the math for the general case of two observers in relative motion, sending each a signal at a predetermined local time. The signals will arrive at the same local time for each.
https://www.physicsforums.com/attachments/51567
 
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  • #98
phyti said:
The signals will arrive at the same local time for each.
Do you think that any reference frame claims otherwise? If not, then no observer is required to use any particular frame to get the correct answer.
 
  • #99
DaleSpam said:
Do you think that any reference frame claims otherwise? If not, then no observer is required to use any particular frame to get the correct answer.

It's intended for bgq, altergnostic, or anyone else who thinks they have to start with a symmetrical situation, i.e. equal speeds in opposite directions.
As for 'frames', I'll wait for a sound/consistent definition, if there is one.
 
  • #100
phyti said:
As for 'frames', I'll wait for a sound/consistent definition, if there is one.
The "official" definition of a frame is given here: http://en.wikipedia.org/wiki/Frame_fields_in_general_relativity

But I usually use the term as though it were synonymous with "coordinate system".

With either definition it should be clear that any observer can use any frame to predict the outcome of any experimental measurement.
 
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