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Einstein's Length Contraction... A problem?! |
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| Sep29-11, 10:16 AM | #1 |
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Einstein's Length Contraction... A problem?!
Hello,
I hope you can help with my question!! I am a 27 year old amateur theoretical physicist about to start a bachelor's degree in physics as a mature student... I have just been going over some bits of Einstein's theory of Special Relativity and have noticed something odd that has confused me! The theory initially states that there is no absolute frame of reference in the universe. Ok, so let's say astronauts Mary and Dave are floating next to each other in space, Dave turns on his jet pack and flies off at 500,000mph. Mary will see Dave as being thinner as he will be experiencing length contraction. So then, shouldn't Dave see Mary as being wider, as in comparison to her, he is thinner?! Instead, it could just have easily been Mary who was accelerated away from Dave, as observers they would still be equal, although in this scenario Dave would see Mary as being thinner! I am confused!! This has also brought about an interesting thought experiment. If someone were to make a million identical metal cubes and blast them off into space in a million different directions at different speeds, then by measuring which one looked biggest couldn't we potentially find a direction of motion (relative to us) that is actually an absolute point in space, i.e. the biggest cube is not actually moving in space? Thank you for your time and help!! |
| Sep29-11, 12:08 PM | #2 |
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Hi, and welcome to Physics Forums!
You're mixing up at least two distinct concepts. Separating them may help to understand what's going on. First, let's remove the jet pack and acceleration from the scenario (we'll put them back in a bit). Suppose Dave and Mary are flying past each other at some large relative velocity; neither one has a rocket engine or any other type of thrust turned on, they are just flying past each other in free fall, both weightless. Then each one will indeed see the other as length contracted. Physically, their situation is completely symmetrical, and there is nothing that picks out either one of them as being in a special state of motion. It may seem confusing that, if Mary sees Dave as thinner, Dave also sees Mary as thinner (instead of wider). But remember that they are flying past each other, and neither of them has any means of changing their speed (no rockets or anything else). So there is no way for them to come to rest relative to one another and actually compare their lengths while they are both in the same state of motion. What Mary sees of Dave is a "projection" of Dave into Mary's state of motion, and vice versa, and because Mary and Dave are moving relative to one another, their states of motion are "tilted" relative to one another. If you learn about spacetime diagrams, they are a good way of making this visually evident, and it becomes obvious that length contraction is just the spacetime version of a projection in geometry. The fact that Mary and Dave each see the other as thinner is then just a geometric consequence of the tilting, just as if I hold up a quarter so that it is face on to me, and you are facing at at angle to me, the quarter will look like a narrowed ellipse instead of a circle, and vice versa if you are holding another quarter face on to you (it will look like a narrowed ellipse to me); our situations are symmetrical, so our experiences are too. Now let's put back the acceleration. Suppose Dave and Mary start out at rest relative to each other, but then Dave turns on his rocket pack and accelerates away. Now there is a real, physical difference between the two: Dave feels acceleration, and is no longer weightless, while Mary remains in free fall and is weightless. Their situations are no longer symmetric. In this particular case, Mary will still see Dave as length contracted, but Dave may be unable to "see" Mary at all while he accelerates, if he accelerates hard enough! That gets into more complications, which you may not want to get into at this stage. But the key is that, if one person is accelerating (i.e., feels an acceleration) and the other doesn't, their situations are not symmetric and the principle of relativity does not require that all of their physical experiences be symmetrical. |
| Oct3-11, 05:07 AM | #3 |
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Oh my god, sorry, of course.....this is the whole point of 'relativity', particularly for this postulate!!! Please do excuse me and thank you for setting me straight :)
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| Feb29-12, 01:31 PM | #4 |
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Einstein's Length Contraction... A problem?!
This apparent paradox used to baffle me as well. A simple analogy, ignoring relativity completely, is how big they would appear to each other. From far way, Mary would see Dave as appearing quite small – he would have a small angular size.
But this, of course, doesn’t mean that Dave would see Mary as being huge – she would appear equally diminished to him. Both are right. And each would believe (rightly) that they had not changed in size at all. A whole bunch of odd things happen together when relativity comes into play. As well as a moving object (e.g. a spaceship) appearing to us to shrink in length, the rate of the passage of time on it appears to us to be slower than it did when it was stationary. Also, time at the front end of the spaceship appears to us to lag behind time at the rear. But the wording is important. To the people on the ‘moving’ spaceship itself, none of these things are apparent about them and their vessel. However, they would rightly argue that it is we who had contracted in length, that our time was running slowly (compared with their ship clocks) and that our clocks, which of course appear synchronised to us, are asynchronised to them. The strange effects of special relativity result from a strict application of the two postulates. Many special relativity paradoxes are resolved when all these effects are considered together – not just one of them. It’s very easy to remember one effect and forget another! |
| Jun29-12, 06:44 PM | #5 |
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The difference is that the one accelerating away will see the "fixed stars" contract. The average velocity of the fixed stars creates a unique frame of reference which comes from the big bang.
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| Jul3-12, 02:48 PM | #6 |
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| Jul3-12, 02:54 PM | #7 |
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| Jul3-12, 04:22 PM | #8 |
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Mentor
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| Jul4-12, 03:46 AM | #9 |
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If your textbook is good, it has a derivation of length contraction based on the Lorentz transformations. The moving length must be determined by comparing it to the length Δx of your ruler - "length contraction" thus refers to the ratio Δx'/Δx at either Δt=0 or at Δt'=0. Check it out and you will probably find that there the moving length Δx' is derived for Δt=0 (simultaneous in system S). Now try to work out how such lengths compare for Δt'=0 (simultaneous in system S') and make a sketch of it.
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| Jul4-12, 06:43 AM | #10 |
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| Jul4-12, 06:58 AM | #11 |
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You are assuming that "simultaneous" makes sense here and it doesn't. Two events happening in two different places can be "simultaneous" to one observer and not to another.
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| Jul4-12, 07:09 AM | #12 |
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| Jul4-12, 10:07 AM | #13 |
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| Jul5-12, 03:00 AM | #14 |
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Mary measures simultaneously between events that are not simultaneous in Dave's world (But Dave measures his train between the for him simultaneous events (f.ex.) 'back says 'L' and front says 'L'). Mary puts cameras along the railwaytrack. The train passes an inch before the camera's. All together the photos make one big picture of the passing train on the railwaytack On the picture the train is shorter because the trazin is indeed shorter. Back of train says 'L' and front says 'K'. What's wrong with this? Were is the mistake? |
| Jul5-12, 06:08 AM | #15 |
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| Jul13-12, 11:01 AM | #16 |
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![]() In Dave's train (orange) somebody at the back of the train and somebody at the front of the train both recite the alphabet simultaneously. Dave measures his train between the brown and purple event; when for him person at the back and the person at the front of the train say 'L'. Notice I have added a tree. From the trainstation Mary measures the moving train between between the purple and blue event; between person at the back saying 'L' and the person at the front of the train saying 'K'. I do not see any projection taking place. There are no events projected from the orange line onto the green horizontal line. F.ex. the brown event 'front of train at tree' is not dropped on the green line and replacing the blue event. Orange and green are rather different 'cuts' through the timelines. 3D cuts though 4D spacetime. I find 'projection' rather confusing terminology. Even wrong. Why? If I project a photo of a train (with the front of a train hitting a tree) to the wall under an oblique angle, the train will be projected shorter, but still hitting the tree. (Similar line of thought can be said about some perspective drawing). So writing for the the layman that lengthcontraction is a 'projection' will never make him understand what relativity of simultaneity is, the crux of special relativity. |
| Jul13-12, 02:14 PM | #17 |
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