I Because of length contraction, does absolute position exist?

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The discussion centers on the concept of absolute position in the context of relativity and its implications for measuring length. It asserts that there is no absolute position in either general relativity (GR) or classical mechanics, as measurements of length depend on the observer's frame of reference. The analogy of slicing a sausage is used to illustrate that different observers measure different lengths of the same object based on their simultaneity conventions. It is clarified that while measurements differ, they do not imply a superposition of positions like in quantum mechanics; rather, they reflect different perspectives on the same four-dimensional object. Ultimately, the conversation emphasizes that measurements are frame-dependent and do not indicate a fundamental ambiguity in position.
  • #31
jbriggs444 said:
Is the meter stick at rest on the sidewalk that Bob is standing on? Or is it at rest strapped to the rocket that Alice is riding on?
The meter stick is at rest on the ground along the x axis. And one end of it is at Bob's feet.
 
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  • #32
Ibix said:
No there is not a superposition. Please read that sentence repeatedly until it sinks in. We have all told you this and the posters at scienceforums.net have told you this. I get that you don't understand what is going on, but desperately hoping that it's actually something every subject expert is telling you it's not is not going to help you.

I can't make sense of your scenario. I think what you are doing is having Bob at rest in some frame and Alice moving at some speed in the +x direction. Two particles also move in the +x direction, at rest with respect to one another. Both Bob and Alice have identical meter rules that they use to measure the distance between the particles.

Let's say that the back particle, Alice, Bob, and the zero end of both their rulers pass at one time (you called this 5pm). To measure the distance between the particles, both Bob and Alice make note of where the front particle is at the same time as the back particle passes them. But they do not have the same idea of what "at the same time" means, so both will say that they measured the front particle's position at time zero, but that the other did not. Thus the other includes some timelike separation in their length measure.

This is what is illustrated in jbriggs444's diagram on the previous page shows - both frames use the same event to measure the location of one end, but use different events for the other end.
The particles are at rest at each end of the meter stick. The meter stick is lying on the ground with one end of the meter stick at Bob's feet. There is only one meter stick, and it is parallel to the motion of Alice flying by at Bob's feet (this is hard to visualize because Alice is practically touching the ground as she travels parallel to the meter stick which is also on the ground.)
 
  • #33
jbriggs444 said:
A meter stick is not a line segment the exists only as a snapshot in time. It has extent in time and is more like a parallelogram extending indefinitely into the past and into the future. When you measure its length, you are taking a snapshot at an instant in time according to some chosen frame.
View attachment 294841
When you measure the length of the stick in frame A, you are measuring from event a1 to event a2 such that a1 and a2 are simultaneous according to frame A.

When you measure the length of the stick in frame B, you are measuring from event b1 to event b2 such that b1 and b2 are simultaneous according to frame B.
Thanks a lot for this. Why is the meter stick longer in Frame B? Is Frame A traveling fast?
 
  • #34
Ok. Then Bob says that the particles are a meter apart and Alice can't make a measurement because she doesn't have a meter rule that is at rest in her frame.
 
  • #35
Ibix said:
Ok. Then Bob says that the particles are a meter apart and Alice can't make a measurement because she doesn't have a meter rule that is at rest in her frame.
But can't we talk about what the distance between the two particles is in Alice's frame of reference?
 
  • #36
student34 said:
But can't we talk about what the distance between the two particles is in Alice's frame of reference?
Sure, but she needs a meter rule too. Both will see the other's meter rule contracted and therefore cannot agree that the front end of the two meter rules will be at the same place at the same time as the back ends are at the same place. Thus they must measure different distances between the particles.
 
  • #37
Ibix said:
Sure, but she needs a meter rule too. Both will see the other's meter rule contracted and therefore cannot agree that the front end of the two meter rules will be at the same place at the same time as the back ends are at the same place. Thus they must measure different distances between the particles.
But I am only interested in where the particle is at the meter stick in front of Bob. This will help me understand how there is no superposition of that particle. It is exactly this scenario that is causing me to think that that particle must be in two different locations in space.
 
  • #38
student34 said:
It is exactly this scenario that is causing me to think that that particle must be in two different locations in space.
It is (edit: at least in some frames), just not at the same time. Thats what jbriggs444's diagram is showing you. Do you understand it? It's really the easiest way to resolve all relativistic weirdness.
 
  • #39
Ibix said:
It is, just not at the same time. Thats what jbriggs444's diagram is showing you. Do you understand it? It's really the easiest way to resolve all relativistic weirdness.
Yeah, I think that diagram will help me. Is one of the frames in motion?
 
  • #40
student34 said:
Yeah, I think that diagram will help me. Is one of the frames in motion?
Yes. In order to get two different simultaneity conventions, the frames need to be in relative motion.
 
  • #41
student34 said:
I am only interested in where the particle is at the meter stick in front of Bob.
Then why do you care what Alice measures? You have already said that both particles are at rest relative to Bob, one at each end of the meter stick. That is a perfectly consistent scenario and there is no "superposition" whatever: each particle has a well-defined unique position relative to Bob and his meter stick.
 
  • #42
jbriggs444 said:
Yes. In order to get two different simultaneity conventions, the frames need to be in relative motion.
In the example given in the diagram, what is happening with the frames? Why is the meter stick longer in Frame B?
 
  • #43
student34 said:
It is exactly this scenario that is causing me to think that that particle must be in two different locations in space.
Why would you think that? Each particle is at one end of Bob's meter stick. And that is just as true for Alice as it is for Bob. The particles are moving relative to Alice and Alice's meter stick will measure a different distance between them, but Alice's meter stick will still measure each particle to be co-located with one end of Bob's meter stick. In Alice's frame each particle just moves in sync with its end of Bob's meter stick, instead of being at rest at its end of Bob's meter stick as it is in Bob's frame. The fact of each particle being co-located with one end of Bob's meter stick is an invariant, and is true in all frames.
 
  • #44
PeterDonis said:
Then why do you care what Alice measures?
Because, for Alice, the particle seems to be in a different location than for Bob. When Alice is at x with Bob, the particle is only 50 cm from Alice. But as others have responded, we are also using Alice's clock, which is at a different time than Bob's.

But my response to that is that Alice's time is just some time t earlier than Bob's clock. And at that time the particles were still 100cm apart for Bob. The particles are never 50cm apart other than for Alice's frame. What else can I think other than some kind of superposition? I just don't understand how this is wrong.
 
  • #45
student34 said:
When Alice is at x with Bob, the particle is only 50 cm from Alice.
"When Alice is at x with Bob" is different for Alice than it is for Bob. Alice and Bob have different notions of simultaneity because of their relative motion.

student34 said:
we are also using Alice's clock, which is at a different time than Bob's.
It's not just that it's "at a different time". It is running at a different rate. To Alice, Bob's clock is running slow; to Bob, Alice's clock is running slow.

In other words, there are actually three frame-dependent effects going on here: length contraction, time dilation, and relativity of simultaneity. And it is impossible to look at just one of these, or even just two, and get a correct picture of what is going on. You have to look at all three in combination. That is what the spacetime diagrams that have been drawn in this thread are doing.

student34 said:
The particles are never 50cm apart other than for Alice's frame.
And they are never 100cm apart other than in Bob's frame. And in any other frame, they would be a different distance apart, and would be moving at a different speed. And the time dilation and simultaneity would also be different.
 
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  • #46
jbriggs444 said:
When you measure the length of the stick in frame A, you are measuring from event a1 to event a2 such that a1 and a2 are simultaneous according to frame A.

When you measure the length of the stick in frame B, you are measuring from event b1 to event b2 such that b1 and b2 are simultaneous according to frame B.
It would probably be better to reverse the frame nomenclature here. The natural way to interpret this diagram is that what you are calling frame A is Bob's frame (since that's the frame in which both worldlines, representing the two ends of Bob's meter stick, are at rest) and what you are calling frame B is Alice's frame.
 
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  • #47
student34 said:
Why is the meter stick longer in Frame B? Is Frame A traveling fast?
Per my post #46 just now, as @jbriggs444 has drawn the diagram, "Frame A" is really what you are calling Bob's frame, and the "Frame A snapshot" is Bob's meter stick at an instant of Bob's time. "Frame B" in the diagram is really what you are calling Alice's frame, and the "Frame B snapshot" is Bob's meter stick at an instant of Alice's time. Because the geometry of the diagram is actually hyperbolic rather than Euclidean, the length of the "Frame B snapshot" is actually shorter than the length of the "Frame A snapshot", corresponding to the fact that Alice sees Bob's meter stick length contracted. And the fact that the "Frame B snapshot" is at an angle to the "Frame A snapshot" corresponds to relativity of simultaneity.
 
  • #48
student34 said:
Because, for Alice, the particle seems to be in a different location than for Bob. When Alice is at x with Bob, the particle is only 50 cm from Alice. But as others have responded, we are also using Alice's clock, which is at a different time than Bob's.

But my response to that is that Alice's time is just some time t earlier than Bob's clock. And at that time the particles were still 100cm apart for Bob. The particles are never 50cm apart other than for Alice's frame. What else can I think other than some kind of superposition? I just don't understand how this is wrong.
If Alice observes one end of Bob's metre stick at her feet at time ##t = 0## and the other end at her feet at a time a fraction of a second later. She might claim that the metre stick has zero length. Why is that wrong?

Observed position of one end of metre stick: ##x_1 = 0##.

Observed position of other end of metre stick: ##x_2 = 0##.

Length of rod ##L = x_1 - x_2 = 0##.

Why is that wrong?
 
  • #49
jbriggs444 said:
Yes. In order to get two different simultaneity conventions, the frames need to be in relative motion.
jbriggs444 said:
A meter stick is not a line segment the exists only as a snapshot in time. It has extent in time and is more like a parallelogram extending indefinitely into the past and into the future. When you measure its length, you are taking a snapshot at an instant in time according to some chosen frame.
View attachment 294841
When you measure the length of the stick in frame A, you are measuring from event a1 to event a2 such that a1 and a2 are simultaneous according to frame A.

When you measure the length of the stick in frame B, you are measuring from event b1 to event b2 such that b1 and b2 are simultaneous according to frame B.
I am sorry everyone; this is embarrassing. I just realized that this diagram is a description of my thought experiment. I understand now what is going on. Thanks a lot for this diagram.
 
  • #50
PeterDonis said:
It's not just that it's "at a different time". It is running at a different rate. To Alice, Bob's clock is running slow; to Bob, Alice's clock is running slow.
I don't think this is correct. Only one of them would have the slower clock. It depends which one did the acceleration from when they were at rest with one another. In this case Alice did the acceleration, and so only Alice's clock is slower.
 
  • #51
student34 said:
I don't think this is correct. Only one of them would have the slower clock. It depends which one did the acceleration from when they were at rest with one another. In this case Alice did the acceleration, and so only Alice's clock is slower.
What if they both accelerated equally in order to achieve their relative velocity? Like both went round the Large Hadron Collider in opposite directions?
 
  • #52
PeroK said:
What if they both accelerated equally in order to achieve their relative velocity? Like both went round the Large Hadron Collider in opposite directions?
I guess both would have slower clocks relative to clocks on Earth, but Alice's would still slower since she would have had to do more of the acceleration to get to a 50% length contraction of Bob's meter stick.

Are you saying that I am wrong about my correction?
 
  • #53
student34 said:
I guess both would have slower clocks relative to clocks on Earth, but Alice's would still slower since she would have had to do more of the acceleration to get to a 50% length contraction of Bob's meter stick.

Are you saying that I am wrong about my correction?
Yes, you couldn't be more wrong, as the saying goes! The Lorentz Transformation is symmetric. There is no "absolutely at rest" frame and no "accelerated and really moving" frame.

That is, in fact, the principle of relativity that dates back to Galileo.
 
  • #54
PeroK said:
Yes, you couldn't be more wrong, as the saying goes! The Lorentz Transformation is symmetric. There is no "absolutely at rest" frame and no "accelerated and really moving" frame.

That is, in fact, the principle of relativity that dates back to Galileo.
So do you also not accept the explanation for the Twins paradox?
 
  • #55
student34 said:
I don't think this is correct. Only one of them would have the slower clock.
This is incorrect. Each one is moving inertially, so each one perceives the other's clock to be running slow.

student34 said:
It depends which one did the acceleration from when they were at rest with one another.
There is no requirement that they ever were at rest relative to one another.

If they started out at rest, and one of them accelerated away, and then turned around and accelerated back, and came to rest again relative to the other, while the other one remained inertial the whole time, then the one who traveled would have less time elapsed on their clock (and both of them would agree about this). But that is not time dilation; that's a "twin paradox" scenario, which is something different.

And, as above, there is no requirement that two people who happen to be moving relative to one another now were ever at rest relative to one another in the past, so not every scenario will even meet the requirements for being a "twin paradox" scenario where there is an invariant (i.e., not frame dependent) answer as to whose clock has more or less elapsed time. In many cases there is simply no invariant answer to that question; all you have is the various frame-dependent answers for each one's frame.
 
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  • #56
student34 said:
So do you also not accept the explanation for the Twins paradox?
Please see my post #55 just now. The scenario we have been discussing in this thread is not the same as the twin paradox scenario.
 
  • #57
student34 said:
Alice's would still slower since she would have had to do more of the acceleration to get to a 50% length contraction of Bob's meter stick.
Even in "twin paradox" type scenarios, this reasoning is not correct. Length contraction is still frame-dependent no matter what the past history of either observer was.
 
  • #58
student34 said:
So do you also not accept the explanation for the Twins paradox?

You are missing what puts "paradox" in "twin's paradox".

i.e. that for both the other has a slower clock (while in relative motion).

The explanation of the twin's paradox is not about one of them "really" having the slowest clock.
 
  • #59
sdkfz said:
The explanation of the twin's paradox is not about one of them "really" having the slowest clock.
Actually, yes, it is. As I said in post #55, the difference in elapsed time on the twins' clocks when they come back together is an invariant, not frame-dependent. So yes, one of them "really" has aged less.
 
  • #60
PeterDonis said:
Actually, yes, it is. As I said in post #55, the difference in elapsed time on the twins' clocks when they come back together is an invariant, not frame-dependent. So yes, one of them "really" has aged less.

Of course one has really aged less, that's the other side of the "paradox". I'm not contradicting that.
 

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