I Because of length contraction, does absolute position exist?

student34
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I know that I have heard that GR proves that there is no absolute time, so does this go for location too?

If so, could it be said that particles have a superposition in position/location the same way that particles do in QM?
 
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There is no such thing as absolute position. Not in relativity nor in classical mechanics.

Note that this is not at all the same issue as that of positional uncertainty in quantum mechanics.
 
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student34 said:
I know that I have heard that GR proves that there is no absolute time, so does this go for location too?
Galileo showed that there was no absolute notion of position, but Einsteinian relativity agrees, yes.
student34 said:
If so, could it be said that particles have a superposition in position/location the same way that particles do in QM?
No. Position and length are well defined. Different frames measure different aspects of a 4d object but both call it length. It's closely analogous to slicing a sausage perpendicular to its length and seeing a circular cross-section and somebody else slicing it diagonally and seeing an elliptical cross section. The sausage is not in a superposition of circular and elliptical - the different people are just making different measurements on it.
 
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Ibix said:
It's closely analogous to slicing a sausage perpendicular to its length and seeing a circular cross-section and somebody else slicing it diagonally and seeing an elliptical cross section. The sausage is not in a superposition of circular and elliptical - the different people are just making different measurements on it.
I am stealing this analogy for future classes. :wink:
 
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Ibix said:
Galileo showed that there was no absolute notion of position, but Einsteinian relativity agrees, yes.

No. Position and length are well defined. Different frames measure different aspects of a 4d object but both call it length. It's closely analogous to slicing a sausage perpendicular to its length and seeing a circular cross-section and somebody else slicing it diagonally and seeing an elliptical cross section. The sausage is not in a superposition of circular and elliptical - the different people are just making different measurements on it.
But wouldn't one of the measurements be of different parts of the sausage than the other?
 
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student34 said:
But wouldn't one of the measurements be of different parts of the sausage than the other?
Yes, because we can’t slice a sausage twice at the same place. That just shows us that the analogy is not exact which isn’t surprising because all analogies are, by definition, not the exact real thing.
 
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student34 said:
But wouldn't one of the measurements be of different parts of the sausage than the other?
Yes. Likewise, two length measurements made using different frames' simultaneity conventions are not made at the same time. Each frame will describe the other frame measurement as having a duration, and its own as being instantaneous. So they measure different sections of the 4d object.
 
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student34 said:
But wouldn't one of the measurements be of different parts of the sausage than the other?
That is the point. Different measurements of length similarly measure different parts of the 4D object.
 
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Orodruin said:
I am stealing this analogy for future classes. :wink:
The same here :-).
 
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  • #10
student34 said:
But wouldn't one of the measurements be of different parts of the sausage than the other?
Say a measure is at rest in an IFR. The two ends draw two world lines in spacetime. Space distance between the lines so to say space distance between the ends depends on in which IFR the observer is. Observers in different IFRs observe the same lines with different space distance. He or she in the original IFR observes the longest distance.
 
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  • #11
anuttarasammyak said:
Say a measure is at rest in an IFR. The two ends draw two world lines in spacetime. Space distance between the lines so to say space distance between the ends depends on in which IFR the observer is. Observers in different IFRs observe the same lines with different space distance. He or she in the original IFR observes the longest distance.
Ok, so for Bob standing next to a meter stick, the particles on the ends of the meter stick are a meter stick apart. For Alice traveling fast, parallel to the meter stick, the meter stick is, say, half the size, and thus the particles are 50 cm from each other.

According to GR, there exist 2 real sizes of meter stick here. How can the particles at the ends of the meter stick possibly be in the same location in space for each frame of reference?
 
  • #12
student34 said:
According to GR, there exist 2 real sizes of meter stick here. How can the particles at the ends of the meter stick possibly be in the same location in space for each frame of reference?
They aren't. The frames don't agree on simultaneity so their measurements of where at least one end of the meter stick is aren't taken at the same time, and the meter stick is moving in at least one frame. So according to each frame at least one end of the rod isn't in the same place when measurements are made by the other frame.

This is the point we've been trying to make to you. What one frame measures as "length" is a different measurement of the object from what the other frame measures as "length".
 
  • #13
student34 said:
According to GR, there exist 2 real sizes of meter stick here. How can the particles at the ends of the meter stick possibly be in the same location in space for each frame of reference?
If you are in a train, looking at your cellphone. To you, your cellphone is stationary. It's not moving and you can operate it easily. To domeone on the platform, your cellphone is moving at 150 km per hour, say.

How can your cellphone be moving and not moving at the same time? How can you and the person on the platform possibly be describing the same physical object?
 
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student34 said:
According to GR….
SR as well. We are running out of ways of saying that the two measurements are of different things.
 
  • #15
Ibix said:
They aren't. The frames don't agree on simultaneity so their measurements of where at least one end of the meter stick is aren't taken at the same time, and the meter stick is moving in at least one frame. So according to each frame at least one end of the rod isn't in the same place when measurements are made by the other frame.
Okay, I hope you don't mind if I try to really nail this down here with the following 2 questions. Is the meter stick truly 50 cm for Alice? Is the meter stick truly 100 cm for Bob?
 
  • #16
Nugatory said:
SR as well. We are running out of ways of saying that the two measurements are of different things.
Let's say that the meter stick is on the x coordinate for Bob's frame of reference. Will the meter stick be on the x coordinate for Alice's frame of reference?
 
  • #17
student34 said:
Okay, I hope you don't mind if I try to really nail this down here with the following 2 questions. Is the meter stick truly 50 cm for Alice? Is the meter stick truly 100 cm for Bob?
Yes. They are measuring the spatial extent of different 3d slices through a 4d object.
 
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student34 said:
Let's say that the meter stick is on the x coordinate for Bob's frame of reference. Will the meter stick be on the x coordinate for Alice's frame of reference?
Do you mean "on the x axis"?
 
  • #19
Ibix said:
Do you mean "on the x axis"?
Yes
 
  • #20
student34 said:
Yes
Then yes, the rod can lie completely in the ##xt## and ##x't'## plane.
 
  • #21
Ibix said:
Yes. They are measuring the spatial extent of different 3d slices through a 4d object.
So the particles exist in the objective universe as being 50 cm apart and 100cm apart. Is that correct?
 
  • #22
student34 said:
So the particles exist in the objective universe as being 50 cm apart and 100cm apart. Is that correct?
50cm along one axis and 100cm along a different axis, yes. That was the point of the sausage analogy - the edges of the sausage are different distances apart if you look along different directions. Similarly, the distance between the particles depends if you measure along Alice's x-axis or Bob's x' axis.
 
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  • #23
student34 said:
Is the meter stick truly 50 cm for Alice? Is the meter stick truly 100 cm for Bob?
Instead of tossing around words like “truly” (what would it mean to say the rod is “not truly”?)we should state the objective facts.

Using Bob’s simultaneity convention the ends of the rod are 100 cm apart. Using Alice’s simultaneity convention the ends of the rod are 50 cm apart. These are facts about which there is no dispute and can (in principle) be measured directly with suitable lab equipment.

So those are the facts. If you want to consider those facts as equivalent to saying “the meter stick is truly 50 cm long for Alice and truly 100 cm long for Bob”, or not….either way it says more about what you mean by “truly” than about the rod.
 
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  • #25
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.
1640719931203.png

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.
 
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  • #26
So, @student34, the diagram in @jbriggs444's post is a spacetime diagram. The x position of something is shown horizontally and the t position vertically. In this frame, then, the length of the rod is the Minkowski interval along the horizontal line. In a different frame with a different x-axis (call this x') which slopes down the page, though, the length of the rod is the Minkowski interval along the sloped line. It isn't the same as the length measured by the other frame, but there's no superposition going on here. The two frames are just measuring along different 1d cross sections of the 2d rod.
 
  • #27
student34 said:
Okay, I hope you don't mind if I try to really nail this down here with the following 2 questions. Is the meter stick truly 50 cm for Alice? Is the meter stick truly 100 cm for Bob?
This is what happens when you unify space and time into spacetime. It's the spacetime interval between events that is invariant; and not both the space interval and the time interval.

If you insist that space and time are distinct and unrelated, then SR will forever remain perplexing and a source of consternation.
 
  • #28
Ibix said:
50cm along one axis and 100cm along a different axis, yes. That was the point of the sausage analogy - the edges of the sausage are different distances apart if you look along different directions. Similarly, the rod.
Okay thanks a lot. This next part will really answer my question about whether or not there is a superposition of position.

Let's say that Alice goes flying past Bob right at his feet causing the meter stick to contract to 50cm. So an x value of Bob's frame will intersect with an x value of Alice's frame as she goes past Bob. And the meter stick is on the x-axis lying in front of Bob with one end touching his feet.

When Alice and Bob were together on the ground before her flight, their clocks were synchronized at say 1:00pm. Alice flies directly over Bob's head at 5:00pm as per Bob's clock.

The particle at the end of the meter stick 100cm from Bob's feet we will call Bf (B for Bob's frame and f for far). So when Alice is at Bob's feet, the particle 100cm from Bob we can say that it is an event at some value Bf(x,y,z,t). And the other particle will be Bc(x,y,x,t) where c is for close. For Alice, similarly, we can use Ac(x,y,z,t) and Af(x,y,z,t)

When Af(x) = Bf(x), Af(z) = Bf(z) right?
 
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  • #29
student34 said:
Let's say that Alice goes flying past Bob right at his feet causing the meter stick to contract to 50cm.
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?
 
  • #30
student34 said:
This next part will really answer my question about whether or not there is a superposition of position.
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.
 
  • #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.
 
  • #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.
 

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