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O2(0.99999999999999999999c)--------> L1 B1--------O1-------B2 L2 M1 M2
So for oberver O2 ball B2 is pulled down about 4 minutes before ball B1 and the chain breaks.So we have a paradox, for observer O1 the chain is intact and for observer O2 the chain is broken.Both situations can't simultaneously be true.
Because information cannot travel faster than the speed of light. A rigid body is one in which the distances between every atom are fixed and do not change. But if we gave such a body a push from one end, information would have to travel through the entire body instantaneously to signal to all other parts of the body to 'move'. This means information has to travel faster than light which is precluded by special relativity. So, rigid bodies cannot be described by special relativity, and therefore do not exist in the physical world.
That's nice. It's also completely irrelevant. Nowhere in the opening post is it stated, implied, assumed, nor required that the transmission of movement along the chain from the movement of the balls must exceed the speed of light.
Anyway, my entire point is that the chain cannot be thought of as being rigid, i.e. it has some flexibility to it whereas you implied that it had to break implying that you're assuming that it's rigid, i.e. that the length doesn't change or if it tried it would break. That's a false assumption.
I don't know about you, but my experience with chains is that they're not very stretchy.
So I guess you're implying that the chain would remain intact for both observers even though the chain would need to increase in length for observer O2?
... as determined by observers in S', the ends of the rod do not start moving at the same time. So even though the rod is absolutely rigid in frame S it isn't as observed in frame S'. This is why it's said that there are no rigid bodies in special relativity.
Absolutely.
But all this doesn't matter because if the chain moved as a rigid body (zero stretching) in frame O1 it will not have that property in frame O2.
You're merely rehashing the opening post. The balls move simultaneously for observer O1, but for observer O2 there is a difference of about 4 minutes.
So your resolution to the paradox is that the chain doesn't break for observer O2 even though it grows in length. This is because the chain is in a different frame of reference.
Now putting aside the ridiculous absurdity of this for a moment, ...
this can't be true because this leads to another unresolvable paradox.
Imagine for a moment that the movement of the balls is not simultaneous for observer O1 and also not simultaneous for observer O2. Now the chain will break for observer O1, but it won't break for observer O2. So I don't see this as a solution.
So how does this give us chains that magically stretch?
When you make silly ridiculous statements I need to point it out.
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Anyway, please stop with the "ridiculous absurdity" talk. It's not very polite and I've been very polite to you throughout this entire discussion. To be honest, when someone says things like that all it tells me is that they have a poor grasp of the physics involved.
When the equations for relativistic quantum mechanics were finally formulated by Dirac, Lorentz's attempt to calculate length contraction from atomic physics had nearly been forgotten, and Dirac nor any of his contemporaries thought to apply his new equations of relativistic quantum mechanics to the problem of length contraction. It wasn't until 1941 when the American physicist W.F.G Swann revisited Lorentz's arguments in the context of relativistic quantum mechanics and showed that, indeed, the length contraction emerges from a quantum-theoretical calculation of the length of a solid body when the length of a moving body is compared with the length of a similar body at rest. Swann's argument also applies to time dilation, and they can be used to show how the internal dynamics of an atom or of any kind of clock lead to a time dilation, that is, a reduction of the frequency of vibration or ticking of a moving atom or a moving clock. But Swann's argument was as quickly forgotten as Lorentz's.
Wow! You have no problem with a body shrinking from Lorentz contraction but insult me when I explain that a similar thing happens for stretching regarding rigid bodies. It "magically" stretches in the same way that a rod "magically" contracts when in motion due to Lorentz contraction. Gee! You never thought of that, have you? This fact about elasticity and there being no such thing as a rigid body, i.e. nothing exists that can't stretch, is a well-known fact and is found in almost all SR textbooks.
Out of all the special relativity textbooks that I have almost all of them explain that rigid bodies don't exist and SR can be used to show why. I'll list six of the occurrences of this in the SR texts that I have, the last of which I'll quote:Relativity; Special, General and Cosmological by Wolfgang Rindler.Basic Relativity by Richard A. Mould.Special Relativity by A.P. French.Introducing Special Relativity by W.S.C Williams.Theory of Relativity by W. Pauli.From Special Relativity: A Modern Introduction by Hans C. Ohanian. From the section entitled The synchronization of clocks and the Relativity of Simultaneity. On page 49 the author writes[/b]Quote from: Hans C. Ohanian
Length contraction is part of Special Relativity.
Einstein (1907b) discussed the question of whether, in rigid bodies, as well as in all other cases, the velocity of information can exceed the speed of light, and explained that information could be transmitted under these circumstances into the past, thus causality would be violated.
But I've never read anything about objects that magically stretch.
Do you have any sources or is this something you just made up?
We need to stick to the theory.
This fact about elasticity and there being no such thing as a rigid body, i.e. nothing exists that can't stretch, is a well-known fact and is found in almost all SR textbooks.
Out of all the special relativity textbooks that I have almost all of them explain that rigid bodies don't exist and SR can be used to show why.
More generally, a physical signal of any kind cannot have a speed exceeding the speed of light. A direct consequence of this limitation is that an absolutely rigid body cannot exist, because such a rigid body could be used to transmit signals with infinite speed. For instance, a sudden push exerted against one end of an absolutely rigid rod would cause an immediate displacement of the other end of the rod, which would constitute a signal with infinite speed. Physical rods made of solid materials are always somewhat elastic. They are stiff but not absolutely rigid, and the speed of a compression signal propagating along the rod depends on the speed of sound in the solid material; this speed is always much lower than the speed of light.
I guess I have to repeat myself.......That's nice. It's also completely irrelevant. Nowhere in the opening post is it stated, implied, assumed, nor required that the transmission of movement along the chain from the movement of the balls must exceed the speed of light.
So what? You missed my point. Besides, I didn't say otherwise. I merely showed you a site that describes why there is not such thing as a rigid body in SR. That it talks about other things is irrelevant.
We will now show that not only the assumption of an instantaneous spread of some effect, but also, more generally, any assumption of the spreading of an effect with a velocity greater than the velocity of light is incompatible with the theory of relativity.
One particular consequence of the physical speed limit equal to c is that the classical concept of an ideal rigid body finds no place in relativity. (And strictly speaking, it cannot be justified in classical mechanics either.) For by a rigid body we mean an object which physical information can be transmitted in an arbitrarily short time, so that the object is set in motion instantaneously, as a single unit, when a force is applied to any point in it. For an ordinary box, the information that one end has been struck is transmitted as an elastic wave, which we know is many orders of magnitude slower than a light signal.
Let there be a rod having zero elasticity (i.e. infinite Young's modulus) lying at rest along on the x-axis in the inertial frame S. Now accelerate the rod in the +x direction. If the rod is perfectly rigid then all parts will move at the same time. Define the following events:Event #1 (E1): Left end of rod starts to accelerate at t = 0Event #2 (E2): Right end of rod starts to accelerate at t = 0What do observers in the inertial frame S' which is in standard configuration observe? Using the Lorentz contraction you determine that the ends don't start moving at the same time because while E1 and E2 are simultaneous in S they are not simultaneous in S'. Since the ends don't move at the same time the length changes and therefore the body is not rigid.
I don't understand the relevance of this to the opening post.
We aren't dealing with a rod of zero elasticity which I thought you already pointed out couldn't exist anyway.
Let there be a rod lying at rest along on the x-axis in the inertial frame S. Now accelerate the rod rigidly in the +x direction. This means that If the we accelerate all parts of the rod with the same acceleration curve. This means that the rod will behave rigidly in frame S, i.e. all parts of the rod will start to move at the same time and will have the same velocity at the same time as observed in S.
Let me see if I can summarize your solution to the opening post...A rigid body doesn't exist because that would require propagation speeds of movement along a material body to be faster than light, which isn't possible.
Therefore materials have some kind of 'stretchiness' to them. Therefore a chain can stretch for nearly 4 minutes without breaking.
Um, yeah right.
But as I pointed out this would just result in another paradox ...
A paradox is a statement that apparently contradicts itself and yet might be true (or wrong at the same time).
But as I pointed out this would just result in another paradox if the movement of the balls for observer O1 weren't simultaneous and also the movement of the balls for observer O2 weren't simultaneous.
I think we're done here.
Next person please...
A Discussion of Special Relativity by Galina WeinsteinFive topics: A rigid body does not exist in the special theory of relativity; distant simultaneity defined with respect to a given frame of reference without any reference to synchronized clocks; challenges on Einstein's connection of synchronization and contraction; a theory of relativity without light, composition of relative velocities and space of relative velocities.
None of what you're posting is relevant to the opening post.
How does the non-existence of rigid bodies in SR enable such things as chains that stretch for nearly4 minutes without breaking?
Can you give a quote from any text that enables one to draw such a conclusion?Or is this something that you just made up? Because I have never read anything that wouldlead me to believe such a thing.
Quote from: FruityloopSo for oberver O2 ball B2 is pulled down about 4 minutes before ball B1 and the chain breaks.So we have a paradox, for observer O1 the chain is intact and for observer O2 the chain is broken.Both situations can't simultaneously be true.Whenever you think that SR is wrong you can be guaranteed that you made a mistake. This happens every single day on the internet by different people. The result is that the person's understanding of SR is incomplete.In this case you're making the false assumption that the chain can be treated as a rigid body. However its a well-established fact in SR a rigid body does not exist in the special theory of relativity. E.g. if you have a rod that's lying on the x-axis in frame S and you start accelerating every single part of the rod at the same time as observed in S then in frame S' which is in standard configuration with S and which is moving in the +x direction the rod will not remain rigid but different parts will accelerate at different rates. In your case the chain stretches as observed by O2.For more on this please see: https://einstein.stanford.edu/content/relativity/q2018.html