Struggles with the geometrical analogy

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The forum discussion centers on the geometrical analogy of time dilation and the twin paradox in special relativity. Participants clarify that while Lorentz transformations are linear, the invariant spacetime interval differs from the spatial length, which is frame-dependent. The conversation emphasizes that the choice of inertial frames is arbitrary and does not affect the physical outcomes of measurements. Ultimately, the discussion highlights the importance of understanding the geometric interpretation of spacetime in relativity, particularly through Minkowski diagrams.

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  • Knowledge of the twin paradox and time dilation phenomena
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  • #31
A.T. said:
Not sure what you mean here. You define simultaneity based on the measurements and some convention, so it "agrees" with the measurements per definition.
I was responding one of your posts which seemed to suggest I was using loose use of the experience as if it was a raw impression.
 
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  • #32
The reference frame doesn't yield measured simultaneity. Simultaneity is used to construct the reference frame.

OK but it it is all relative and does not change that insistence that the frame in which I am stationary does not have special significance to me does not seem reasonable to me.
 
  • #33
But if someone had carefully synchronized the clocks in any of those other frames, you'd have the same requirement imposed on your frame.

In order to appreciate someone else's experience (measurements) I have to have to perform a transformation. In order for someone else to appreciate my experience they have to perform a transformation. That's relativity.
 
  • #34
Similarly, even simultaneity is not something you experience.
Some have interpreted experience kind of as you have and some interpreted it as I intended. By, experience I do not mean a raw impression but to include calculations based on my understanding of physics. Even I have not yet received a raw, when I do receive it and process it I may come to the conclusion that it happened simultaneously with an event I knew of previously and reason is that it happen at a far distant place.

My understanding is that I can apply frames of reference in which something is moving, which could be me, and a frame of reference in which that thing is stationary. I can personalise the frame of reference in which I am stationary because it relates to my experience and I call that my frame of reference. By experience I mean measurements of space and time, including calculations taking due account of time delays inherent in simple raw observation. Those measurements are the values of the variables of space and time in my frame. Other people would have different personalised frames of reference in which they are stationary. Transformations, between different personalised frames account for different experiences, part of which is the consideration of simultaneity; that is, whether events are simultaneous depends on the frame. Inanimate objects do not personalise, but we can relate to their parameters in our individual personalised frame in which we are stationary.Have I misconceived relativity?
 
  • #35
whatif said:
By, experience I do not mean a raw impression but to include calculations based on my understanding of physics. ... By experience I mean measurements of space and time, including calculations taking due account of time delays inherent in simple raw observation.
That doesn’t salvage your argument at all. Your claim was that “my rest frame is my experience”. I showed that it is not with the usual meaning of experience. With this meaning there is still no frame that uniquely represents my experience since I can do “calculations based on my understanding of physics” in any frame.

So either the claim that “my rest frame is my experience” is wrong because it is not your (raw) experience or it is vacuous since any frame is your (calculated) experience.

whatif said:
insistence that the frame in which I am stationary does not have special significance to me does not seem reasonable to me.
Nevertheless, that is essentially a direct result of the first postulate.
 
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  • #37
whatif said:
OK but it it is all relative and does not change that insistence that the frame in which I am stationary does not have special significance to me does not seem reasonable to me.
Have you ever tried docking a powerboat in a stiff wind? Words fail me in trying to describe the complete insignificance of the frame in which I am rest when dealing with that problem.
 
  • #38
whatif said:
OK, so how do I know what values to apply in any particular frame?
That’s a pretty vague question. The corresponding vague answer is you apply the values that are correct for that particular frame.

If you can make a less vague question then I can probably make a less vague answer. But I have lost the point of this discussion altogether.

If you don’t like the analogy then you are free to not use it. Your opinion against it is valid, your arguments against it are not.
 
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  • #39
whatif said:
OK, so how do I know what values to apply in any particular frame?
See if you can get hold of a copy of Taylor and Wheeler's book "Spacetime Physics". The early chapter explaining exactly what a reference frame is (and equally important, is not) covers this question well.
 
  • #40
See if you can get hold of a copy of Taylor and Wheeler's book "Spacetime Physics".
Got it, assuming “Spacetime Physics Introduction to Special Relativity” is what you meant. I note, as is typical, the examples/problems relate to comparing parameters of observers in different frames of reference with each observer stationary with respect to their frame; consistent with what I have been writing.

Words fail me in trying to describe the complete insignificance of the frame in which I am rest when dealing with that problem.
So you choose to analyse the problem when your frame is comfortably inertial. Forces can be different in different frames. Forces are valid for that frame in which they are analysed. Sure you can analyse the problem in any frame you like and get a valid result for that frame (for the observer in that frame). What forces did you experience as a first-hand observer docking the boat? You seem to contend that is not a meaningful question but it seems to me that if I do the measuring of parameters then the values I measure in the frame in which I am stationary are the appropriate valves for that frame. My reasoning is that I am the observer in that frame of reference and that is my experience.
 
  • #41
whatif said:
My reasoning is that I am the observer in that frame of reference and that is my experience.
A frame of reference is a choice of how to interpret your experience. You are not "in" any frame of reference. Your experience is not a frame of reference.
 
  • #42
whatif said:
What forces did you experience as a first-hand observer docking the boat?
The forces someone directly "experiences" are frame invariant. Analyses in all frames must agree on those.

But note that the term "observer" is often used as a synonym for reference frame, and then "to observe" can also mean "measure frame dependent parameters", rather "direct frame invariant observation".
 
  • #43
OK my experience is not a frame of reference and I and not in a frame of reference but I am referring to frames in which I am represented as stationary. I am the equivalent of the observer for that frame and the measurements I take are the values for that frame. That is my experience, it relates directly to values of things represented in that frame.
 
  • #44
The forces someone directly "experiences" are frame invariant. Analyses in all frames must agree on those.

“The Principle of Relativity does not deny that the force acting on an object is different as reckoned in two frames in relative motion.” Page 59 of my copy of the book. If that is incorrect then I picked a bad parameter.
 
  • #45
whatif said:
I am the equivalent of the observer for that frame
Again, and this cannot be repeated enough, there is no such thing as "an observer for a frame". Your understanding of relativity is lacking and you seem to be interpreting things that people tell you not as they are written, but as they fit within your own ideas. I do not think this is a good way of learning.
 
  • #46
Your understanding of relativity is lacking and you seem to be interpreting things that people tell you not as they are written, but as they fit within your own ideas. I do not think this is a good way of learning.

My understanding of relativity may be lacking but that is an unfair claim and declaratory statements that I am wrong are not explanations. Never mind, I can do simple problems as presented in, say, the book to which I was referred, I get that resolutions in (or should I say by use of) all frames are valid for the specific frame used, I get that spacetime intervals are invariant of the frame used and I get the resolution of the twin paradox using a Minkowski diagram. However, I have lost interest in being enlightened.
 
  • #47
whatif said:
I can do simple problems as presented in, say, the book to which I was referred
That is more useful for understanding, than arguing about words.
 
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  • #48
whatif said:
as is typical, the examples/problems relate to comparing parameters of observers in different frames of reference with each observer stationary with respect to their frame; consistent with what I have been writing.
Typical, yes. Required, no. The first postulate is clear on that. There is nothing special about any frame, you can use the one where you are at rest, but it is not privileged. The use of an observer’s rest frame is a matter of convenience only. Because it is convenient it is commonly done. The first postulate allows this convenience but makes it clear that it is not mandatory.

whatif said:
My reasoning is that I am the observer in that frame of reference and that is my experience.
Which I have shown to be incorrect regardless of how “experience” is interpreted.

whatif said:
What forces did you experience as a first-hand observer docking the boat?
Are you asking about raw experience or calculated experience? If you are asking about raw experience then that would be the frame invariant four force e.g. as directly measured by an accelerometer. From that frame invariant raw four force you could calculate the frame variant three force in any frame.
 
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  • #49
A.T. said:
That is more useful for understanding, than arguing about words.
Thank you.
 
  • #50
Which I have shown to be incorrect regardless of how “experience” is interpreted.
Your have claimed it but I do not think you have shown it.

How does experience relate to frames of reference? What is the reality associated with a frame of reference? It is all very to say the any chosen frame is valid but so is the question and to write the question off because of the way it is handled by geometry and analogues with space alone (which seems to me what you are effectively doing) might be presumptuous. Take the resolution of the twin paradox for example. It has a resolution and they agree, as I see it, because the number of ticks of the identical precise clocks that they carry in their pockets are different by a specific amount. Each clock is stationary for the respective twin (and measures proper time for that twin, as I understand proper time). This is agreeing that one has had more experience, so to speak, than the other, if time is a measure of experience.

The use of different frames may yield a different number of ticks for any person but the experience of time is the same for that person and the rate of ticks of perfect clocks in a persons pocket is does not vary for that person; as I see it.

Anyway, as A.T. suggests that it may be a matter of semantics, or definitions and/or it takes 2, or more, to argue.
 
  • #51
whatif said:
Your have claimed it but I do not think you have shown it.
Sure I did. In 66 I showed that experience does not relate to the reference frame for what you called raw experience. Then in 71 I showed that for your calculated experience it applies to all reference frames equally.

whatif said:
How does experience relate to frames of reference?
As I showed above, raw experience relates to the past light cone rather than your reference frame, and your calculated experience relates equally to any frame of reference.

whatif said:
It is all very to say the any chosen frame is valid but so is the question and to write the question off because of the way it is handled by geometry and analogues with space alone (which seems to me what you are effectively doing) might be presumptuous.
The question was not written off, it was answered. You just didn’t like the answer.

Frankly, it is somewhat irritating to me to provide a substantive answer to your question, have you not respond to the substance of the answer, and then
1) claim that I hadn’t shown what anyone can read and see that I did show
2) say that I “wrote off” a question which I in fact had answered
3) call me presumptuous for the non-existent write off

Really, do you think that is acceptable? If you don’t like or don’t agree with the answer that is one thing, but to claim that you were dismissed or not answered is clearly untrue. Perhaps you were overwhelmed with the volume of responses and could not make a substantive response to mine. That is fine and understandable, but it is also the exact opposite of writing the question off.

whatif said:
one has had more experience, so to speak, than the other, if time is a measure of experience.
Ok, so now you have introduced a third meaning of experience. The time that would be related to someone’s experience is called proper time. Proper time is invariant so all frames agree on it. It does not single out any frame as special.

So now we have three meanings of “experience”. Raw experience depends on the past light cone. Calculated experience could equally apply to any frame. Proper time experience is frame invariant. So none of the three meanings of experience uniquely implies the observer’s rest frame.

whatif said:
the experience of time is the same for that person and the rate of ticks of perfect clocks in a persons pocket is does not vary for that person; as I see it
That is correct. This quantity is called proper time and it is invariant. All reference frames agree on it. Proper time is the Minkowski invariant geometric quantity that is analogous to the Euclidean invariant geometric quantity of length. Your “as I see it” comment actually indicates that you are not too far away from the geometric analogy. You just need to make the connection between your comment above and the analogy.
 
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  • #52
It seems to me that comparing 2 frames in which the objects of interest are represented as stationary, in their respective frames, represents the comparative difference of how all things are experienced in reality. That is, it is not just a different interpretation of reality, it is a different real experience. If not, then I would like to know why not?

With respect to special relativity and inertial frames:
  1. The laws of physics apply to all frames. All frames are valid. The laws of physics have no preference for any particular frame.
  2. It seems to me that frames in which objects are stationary are special with respect to the object of interest, especially when the object is a person.
I see no conflict between 1 and 2. However, 2 seems to be frowned upon because of 1, even though frames in which objects are at rest are typically chosen for analysis; so far as I have seen. I would like to understand why.

Is this explained anywhere?
 
  • #53
whatif said:
It seems to me that comparing 2 frames in which the objects of interest are represented as stationary, in their respective frames, represents the comparative difference of how all things are experienced in reality. That is, it is not just a different interpretation of reality, it is a different real experience.

The word "frame" unfortunately has multiple meanings which imply different answers to this.

First, a word change: the word "experience" is not a good one to use here. I will use "measurements" instead, because we are not (or should not be) talking about subjective opinions of people, but about objective measured quantities that everyone can agree on.

The more common usage is to use "frame" to mean "coordinate chart". (This is more or less the usage in the other open thread you have on this general topic.) A coordinate chart is not (more precisely, does not have to be) a description of anyone's measurements. It is just a mathematical convenience: we assign four numbers to each event in spacetime, with certain requirements on continuity, differentiability, etc. (for example, the numbers describing events that are near each other in spacetime should not differ by much). The numbers do not even have to describe "space" and "time" the way the usual coordinates used for pedagogy in special relativity (global inertial coordinates) do. They can be any numbers whatever that meet the mathematical requirements.

However, there is another, less common usage of "frame", to mean what is more correctly called a "frame field". This is an assignment of four unit vectors, one timelike and three spacelike, to every event in spacetime (again with requirements about continuity, etc.). These vectors represent, heuristically, a clock and three mutually perpendicular rulers that are used by an observer at a given event in spacetime to make measurements. So different frames in this sense represent different physical measuring devices, and therefore different measurement results, i.e., something actually physically different, with the difference being observable.

It's easy to cause confusion in relativity discussions by confusing the above two meanings of "frame".

(Note, btw, that "inertial frame" has meaning in both senses; in the first sense, it means an inertial coordinate chart, i.e., a chart in which objects moving in free fall have worldlines that are straight lines; and in the second sense, it means an assignment of unit vectors at every event such that they are also the basis vectors of some inertial coordinate chart at that event, i.e., they "point" in the four coordinate grid directions at that event.)

whatif said:
The laws of physics apply to all frames. All frames are valid. The laws of physics have no preference for any particular frame.

This is correct, for both senses of "frame" above.

whatif said:
It seems to me that frames in which objects are stationary are special with respect to the object of interest, especially when the object is a person.

Only in the sense that it is often convenient for a person to choose a frame in which they are at rest in order to describe measurements. But that is a matter of convenience, and is not even always true. For example, when you go to the grocery store, do you adopt a frame in which you are at rest? If you do, that means you think of your footsteps on the ground, or the wheels of your car, as moving the Earth and everything on it while you stand still. Is that how you think of it?

whatif said:
I see no conflict between 1 and 2.

There isn't if 2. is interpreted as I did above. But many people (including, I think, you in your other open thread) try to interpret 2. to mean more than I said it did above. The correct response is to not do that.
 
  • #54
Thank you. I do not fully understand, and I won’t labour these points further to making these comments.

There must a connection with reality to apply the physics.

The more common usage of frames, as described, seems to be a purely abstract exercise. I cannot envisage the practical application. That is, for a practical application the numbers must measurable in some way, no? I do not need to know what it is but that it is true.

So different frames in this sense represent different physical measuring devices, and therefore different measurement results, i.e., something actually physically different, with the difference being observable.

I am wondering about the translation. For example, if 2 circumstances are measured with the same device and then again with a different device then the use of either device will detect a physical difference. Otherwise a transformation is required between the measurements to relate them to a common base.

First, a word change: the word "experience" is not a good one to use here. I will use "measurements" instead, because we are not (or should not be) talking about subjective opinions of people, but about objective measured quantities that everyone can agree on.

I understand but the subjective experience must contain a fixed physical influence, in terms of the values of the measurements. So experience can be restricted to the values of the measurements for the purpose, no?

If you do, that means you think of your footsteps on the ground, or the wheels of your car, as moving the Earth and everything on it while you stand still. Is that how you think of it?
I can and have but that situation still involves a comparison between 2 frames in which the objects are considered at rest in their respective frames. It does not describe a different scenario.

Only in the sense that it is often convenient for a person to choose a frame in which they are at rest in order to describe measurements.
Also in the sense of proper length and proper time, no?
 
  • #55
whatif said:
There must a connection with reality to apply the physics.

The connection with reality is the measurable numbers. That's why the first postulate is so important: what it amounts to is that you can calculate the measurable numbers any way you like, because all ways will give the same results. If you're not comfortable with one way, you can just use another, with confidence that you will still be getting the same answers.

whatif said:
The more common usage of frames, as described, seems to be a purely abstract exercise. I cannot envisage the practical application.

Quite possibly not, since you appear to have only a "B" level knowledge of the subject. But note carefully that I pointed out that, for the special case of inertial frames in special relativity, the two usages are basically the same: there is a one-to-one correspondence between frames in the first sense (global inertial coordinate charts) and frames in the second sense (sets of four unit vectors at each event). This sort of correspondence is what Einstein, for example, was referring to when he talked about "frames" as being sets of measuring rods and clocks. Seeing practical applications of such constructions is the purpose of most of the homework problems presented in a textbook such as Taylor & Wheeler's Spacetime Physics.

At more advanced levels, the practical applications of coordinate charts are probably easier to see. For example, in General Relativity, where spacetime can be curved, there are no global inertial coordinate charts, and no global inertial frames in the second sense corresponding to them. And it is often easier to see things like the causal structure of a curved spacetime by coming up with well chosen coordinate charts, even if it is impossible (or at least very difficult) to construct a frame in the second sense that "matches up" with the chart.

whatif said:
if 2 circumstances are measured with the same device and then again with a different device then the use of either device will detect a physical difference.

If the circumstances are physically different, yes. Your description is too general to know. A specific concrete example would help.

whatif said:
Otherwise a transformation is required between the measurements to relate them to a common base.

Transformations are for enforcing the first postulate, that the measurable numbers are the same regardless of which frame you choose. So if you and I both want to calculate the same measurable number (say, the reading on the clock in the tower of Big Ben in London at the instant that the doors of Parliament open on a particular day), and we are using different frames, the frame-dependent quantities in our different frames must be related by certain transformations in order for our answers for the measurable number to both come out the same.

This may be what you are trying to say here; I'm not sure.

whatif said:
the subjective experience must contain a fixed physical influence, in terms of the values of the measurements.

If "fixed physical influence" means objectively measurable quantities, then the effect those quantities have on anyone's subjective experience is outside the domain of physics; it's in the domain of psychology or neuroscience or cognitive science or something like that. Trying to fit it into your understanding of physics is only going to cause problems for you.

whatif said:
So experience can be restricted to the values of the measurements for the purpose, no?

If you want to use the word "experience" this way, I suppose I can't stop you, but I think it is just going to cause problems because you won't be able to resist the temptation to think of it as something subjective. I would recommend avoiding the word completely when you are discussing physics, at least until you have a much better understanding.

whatif said:
I can and have

Really? When you go to the grocery store, you think of yourself as staying still and the Earth and everything else as moving?

whatif said:
Also in the sense of proper length and proper time, no?

You don't need to use a frame in which you are at rest in order to calculate your proper length and proper time. You still are missing the point of the first postulate: you can use any frame you like to calculate any measurable quantity.
 
  • #56
whatif said:
The more common usage of frames, as described, seems to be a purely abstract exercise. I cannot envisage the practical application.

Actually, I forgot to point out a key property that frames in the first sense have (coordinate charts) that frames in the second sense do not have: using a particular coordinate chart doesn't commit you to modeling a particular set of measuring devices, whereas choosing a frame field does. So, for example, if you and I are using different coordinate charts, we can still use them to calculate the same measurable number: our calculations will have different intermediate numbers in them (the frame-dependent quantities), but they will give the same final answer. But if you pick one frame field and I pick another, strictly speaking, we are picking two different measuring devices to model, so we are not going to be able to calculate the same measurable numbers. There are ways around this, but they are much less straightforward than the machinery of coordinate charts. That's why coordinate charts are so much more commonly used and why the standard usage of "frame" refers to coordinate charts.
 
  • #57
A frame, in its usual usage, is a map of spacetime (or, at least, a decision on how to draw one). As with any map, it's usually easiest to interpret if you arrange it so that it somehow reflects your present circumstances (the direction you are facing is up the page, your rest frame), but it's certainly not obligatory to do so. And in any case, the map will never look like what you see. A sufficiently detailed map will allow you to deduce what any given observer would see (that's what Google Street View does) but the map doesn't show that.
 
  • #58
Really? When you go to the grocery store, you think of yourself as staying still and the Earth and everything else as moving?
Yes, really. It not what I typically do but is a thought exercise that I have done.

You don't need to use a frame in which you are at rest in order to calculate your proper length and proper time.
Calculate, yes. However, the definitions that I have come across for proper length is the length of an object measured by an observer which is at rest relative to it.
Proper time is more involved but, as I understand it, a particular application is that if two events happen at the same location using an inertial frame then the spacetime separation between the events is completely timelike and the proper time. Is that correct?
 
  • #59
This may be what you are trying to say here; I'm not sure.
I believe so. The point is that you need some kind of transformation. Also, if each uses a different measuring device then I do not know what you are trying to say unless there is a relationship between the measurements of each device.
 
  • #60
whatif said:
It seems to me that frames in which objects are stationary are special with respect to the object of interest, especially when the object is a person
This is such a weak claim that it can easily be made to be true. All you have to do is define “special” such that it is true.

whatif said:
That is, it is not just a different interpretation of reality, it is a different real experience. If not, then I would like to know why not?
First you need to fix your definition of experience. So far there have been three, and none of them single out the rest frame. You keep moving the goalposts, which is not acceptable. Choose your definition clearly and let’s discuss.

My personal preference is to use the word “measurements” instead as a means of eliminating the subjective aspect. @PeterDonis recommend that and I think it is a good idea too.
 

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