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**Confused about "Aether"**

What is Aether supposed to be now days (and in Einstein's day)? Isn't Aether just space and time (and maybe their fluctuations)?

I thought it was simply a "media", which bosons and fermions travel on.

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What is Aether supposed to be now days (and in Einstein's day)? Isn't Aether just space and time (and maybe their fluctuations)?

I thought it was simply a "media", which bosons and fermions travel on.

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The general belief is that there is no aether.

Somewhat analogously i think space and time can be kind-of seen as a aether - but the big difference is that space-time we know know to be a very dynamical entity -> i.e. it still doesn't depict any absolute reference frame. A theoretical aether (again we don't think there actually is one) would be a medium, not the phenomena or fluctuations through/in/on/with that medium.

I think there are some theories that suggest there is some sort of aether or another; in general, there will always be some theory that predicts there is some sort of everything.

There is no experimental evidence to confirm or (to my knowledge) even suggest an aetheral existence.

I think it is interesting to note however, that because of quantum entanglement, there might be some sort of inextricable link between "distant" parts of space.

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jtbell

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See the FAQ on the http://www.edu-observatory.org/physics-faq/Relativity/SR/experiments.html" [Broken]. Section 2 lists aether-related experiments that were done before Einstein, and Section 3 lists experiments that have been done since then.

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Unfortunately these theories don't really attempt to reconcile such pesky concepts like Lorentz-invariance. For example, they say that, within a Planck Time, random particles can pop in and out of the vacuum without violating conservation of energy. But if vacuum fluctuations are occuring in less than a Planck Time in one observer's frame, what is occuring in the frame of a relativistic traveller, who believes other people's clocks are running slower (and hence, longer than a Planck Time)? Is conservation of energy being violated for some but not others? It's obviously absurd.

Thus I don't think any aether theory is useful for anything other than a mathematical model.

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The reason virtual particles are allowed to "pop" into existence is because of the uncertainty principle -> i.e. DelP*DelT > h or so. And make sure to note that DelT goes (very roughly, and only in the general case - but adequate for us) inversely proportional to T.

Say for instance, in a virtual particles rest frame it "exists" for 10^-15s; If you are moving relativistically relative to the virtual particle, is that time going to increase or decrease (in your moving perspective)?

Now that you've answered "decrease," you see that the uncertainty principle holds even better in a moving reference frame.

The aether has absolutely been REPLACED by field theory (numerous kinds); field theory is not an adaptation of aether - its not building off of the same thing; its a replacement. The aether theory is useless, and none-nonsensical MATHEMATICALLY, and although it probably shouldn't be used at all - it might be somewhat useful to still imagine that there still is an aether, for introductory physics students.

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Um, I would have answered increase. Time 'dilates' - the moving clock runs slower. So in my moving perspective, the particle that exists for 10^-15s from earth's perspective exists for quite a bit longer in my timeframe.Say for instance, in a virtual particles rest frame it "exists" for 10^-15s; If you are moving relativistically relative to the virtual particle, is that time going to increase or decrease (in your moving perspective)?

Now that you've answered "decrease," you see that the uncertainty principle holds even better in a moving reference frame.

It's the same idea as muons decaying more slowly as they bombard the atmosophere because they're moving so fast. They're existing for much longer than they "should." So in a moving frame, a virtual particle on earth could exist longer than it should.

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This is incorrect, muons always decay at the same rate, how a muon moves in relation to an observer is obviously not going to make any difference. It is one of the first principles of the theory of relativity that the laws of physics are the same in all inertial frames of reference, and that includes the (average) time it takes for an elementary particle to decay.It's the same idea as muons decaying more slowly as they bombard the atmosophere because they're moving so fast. They're existing for much longer than they "should." So in a moving frame, a virtual particle on earth could exist longer than it should.

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Anyway; i explicitly said a moving observer and stationary virtual particle.

If you say that the particle is moving at relativistic speeds, then you have additional issues because its energy is drastically increased. If its energy is drastically increased to a stationary observer, then it must exist much shorter than the same particle also stationary. Because its existing for a shorter period of time in the stationary reference frame, its existing longer in its own frame -> corresponding to its smaller energy in its own frame.

And bingo, lorentzian invariance is preserved.

Cheers

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You are completely contradicting yourself here.Of course the laws of physics are invariant... thats the exact reason why muons decay slower when they are moving relative to the observer.

Fact is that observers in relativity all have their own proper time, and one observer's elapsed proper time is not necessarily the same as another. But that does not imply that physical processes go slower. They all go at a rate of one second per second.

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While what i said might be a blatant contradiction to the laymen; it is of course logical to those who have explore the thought experiment derivations of special relativity. For physical laws to be invariant under Lorentz transformations, there must be discontinuity (although superficial) between observers in different reference frames.

Physical processes most certainly do go slower in a moving reference frame, relative to a stationary one. If for no other reason, this is implied by fundamental nature of the speed of light, and the observational truth that all gauge bosons travel at that speed. If photons (w and z bozons, gravitons, and gluons) travel at the same speed - invariant of reference frame - then the E&M (weak, gravity, and strong) forces must act more slowly in moving reference frames.

All physical processes are governed by these forces (if you didn't know), therefore, all physical processes are slowed in moving reference frames.

Note the longer lifetime of particles in particle accelerators; q.e.d.

"They all go at a rate of one second per second" is the moot-point to end all moots! Thats the kind of argument a social studies major would give.... For instance, if you look up the scientific definition of a second... its defined relative to the actions of light, or the vibrations of crystals depending on your source and time period -> both of which are determined by the local reference frame --> therefore a second is not always a second, and a rate of ___ per second is not always ___ per second. But you are right, in one reference frame, one second will be one second (example, try checking your clock, then checking it again).

peter: look into the casimir effect or hawking radiation as evidence of virtual particles "popping".

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It just means that one clock's one path in spacetime was longer than the other. The path length in spacetime between two events is the amount of accumulated proper time.

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einstein concluded that, indeed, there is an ether under GR, which he explained in a paper from 1920. you can read it here: <crackpot web site deleted>

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jtbell

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http://www.ibiblio.org/ebooks/Einstein/Sidelights/Einstein_Sidelights.htm

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A rate is a ration of measurements. If the ratio of measurements are different (clearly, as you say for instance with longer / shorter paths - noting that the other measurement is the constant speed of light) then the rates are different. q.e.d.

It just means that one clock's one path in spacetime was longer than the other. The path length in spacetime between two events is the amount of accumulated proper time.

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Only ether theorists stick to the idea of an absolute time. In relativity there is no absolute time, it is simply nonsense to say that one clock goes slower than another clock al properly working clocks go at the same rate.

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You are self-contradicting MeJennifer. You say that there is no absolute time in relativity, which is true, but afterwards you say that all working clocks go at the same rate? That is exacty what absolute time is, that all clocks go at the same rate.

Two "properly working" clocks that are moving relative to one another will not go at the same rate. I think what you're basically saying is that a clock relative to itself will always tick at 1 sec per second, which is quite obvious..

Two "properly working" clocks that are moving relative to one another will not go at the same rate. I think what you're basically saying is that a clock relative to itself will always tick at 1 sec per second, which is quite obvious..

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That is not a contradiction.You are self-contradicting MeJennifer. You say that there is no absolute time in relativity, which is true, but afterwards you say that all working clocks go at the same rate?

You obviously do not realize that events in spacetime are separated in 4 dimensions. If two observers go from A to B in a different way they could record a different amount of elapsed time for instance in the case of the twin pseudo-paradox. Not because one of the clocks went slower but because it simply took less time to go to B for one observer.

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I'm quite aware, that events in spacetime are separated in 4 dimensions.. I'll try writing what I get from what you're saying.

We're looking at two events A and B from two different frames, S and S' where S is stationary relative to us. If we look at the twin-"paradox" A can be the departure of the spaceship from the earth, and B can be the arrival back at the earth. The two events A and B are colocal in both S and S', they happen at the same place but are separated by a certain amount of time. And then you're saying that the difference in the elapsed time of the journey is due to the fact that the twin in the spaceship travelled a longer spatial distance than the one staying behind?

We're looking at two events A and B from two different frames, S and S' where S is stationary relative to us. If we look at the twin-"paradox" A can be the departure of the spaceship from the earth, and B can be the arrival back at the earth. The two events A and B are colocal in both S and S', they happen at the same place but are separated by a certain amount of time. And then you're saying that the difference in the elapsed time of the journey is due to the fact that the twin in the spaceship travelled a longer spatial distance than the one staying behind?

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Actually the twin in the spaceship traveled a **shorter** path length in spacetime between the two events they have in common, hence the total accumulated time on his clock is less than that of the twin who stayed on Earth who has the extremum path length. His accumulated time is less which does not imply his clock went slower he just experienced less time.

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The formula is: t = T*sqrt(1-(v/c)^2) where t is a proper-time interval and T is the coordinate time interval.

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Ok guys,

Consider this (u might have come across this by the way!)...

There are two frames of reference S and S', in relative motion with velocity v. As none of them can be considered stationary (principle of relativity, all frames are equivalent), how can we choose wether the time is slowed down in S or S'? We can not. However, If we are in S, clock in S' would be slow for us (observer), however, if one of us is in S' instead, for him, our clocks are slow. That means, both clocks are slow, for the observer in other frame. However, that does not mean, that, any watch has actually slowed down due to it's speed. I think that's the point Jeniffer is trying to make (and is correct by me).

In fact, it is absurd to say that, "moving clocks slow down"! In SR, you can not say that any thing is moving. It is impossible to judge at all, wether anything is moving or not. The movement simply means motion relative to observer, and hence either the observer is moving or the event being observed is moving.

regards,

Mitesh

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Ken G

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I also agree with **MeJennifer**, and with **mitesh9's** effort to achieve rapprochement, on the topic of "slowing clocks", that it is in many ways a cleaner picture to simply say that a clock that measures less time actually experienced less time-- the rate of ticking being the same as it always is for good clocks. However, before we get too deeply into arguing that point, we'd better make sure we are distinguishing some pretty important issues.

There are two very different situations where one may wish to compare times. One is when both clocks of interest are inertial, so we expect all of special relativity to apply, but then the two clocks cannot both begin and end their journeys at the same two events (and get anything interesting). So we will always run into the issue of comparing times between different events, and thus we must take care we are not just talking about some arbitrary*coordinatization* (typically, we will be). We will probably use the Einstein simultaneity convention, but when we come up with different numbers for times elapsed, what does that actually mean that isn't just a function of our simultaneity convention?

Alternatively, we could talk about two clocks that make journeys between the same two events, so there is an obvious way to compare the times elapsed, but then at least one of the clocks must be noninertial (to get anything interesting). That means we must apply special relativity with utmost care, because in its rawest form, special relativity must be applied to inertial clocks. The way that's normally done is to track what the noninertial clock is doing by linking it to a succession of inertial clocks that share its motion briefly, but note since these clocks are continually changing, they must still be synchronized somehow, and so we still do not avoid the problem of coordinatization.

In short, it is very easy to think you are arguing physics in this kind of situation, when in fact you are just using a different way of coordinatizing and mistaking the results for something real that can be argued. In my experience, when that is the case, both parties can be perfectly correct, sound like they are completely at odds, and really just be arguing a personal preference for how to look at things. This may be the deepest of all the lessons of relativity, and I do believe that is happening above, for example.

There are two very different situations where one may wish to compare times. One is when both clocks of interest are inertial, so we expect all of special relativity to apply, but then the two clocks cannot both begin and end their journeys at the same two events (and get anything interesting). So we will always run into the issue of comparing times between different events, and thus we must take care we are not just talking about some arbitrary

Alternatively, we could talk about two clocks that make journeys between the same two events, so there is an obvious way to compare the times elapsed, but then at least one of the clocks must be noninertial (to get anything interesting). That means we must apply special relativity with utmost care, because in its rawest form, special relativity must be applied to inertial clocks. The way that's normally done is to track what the noninertial clock is doing by linking it to a succession of inertial clocks that share its motion briefly, but note since these clocks are continually changing, they must still be synchronized somehow, and so we still do not avoid the problem of coordinatization.

In short, it is very easy to think you are arguing physics in this kind of situation, when in fact you are just using a different way of coordinatizing and mistaking the results for something real that can be argued. In my experience, when that is the case, both parties can be perfectly correct, sound like they are completely at odds, and really just be arguing a personal preference for how to look at things. This may be the deepest of all the lessons of relativity, and I do believe that is happening above, for example.

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I agree with you MeJennifer, and Ken G that clocks don't "mechanically" slow down, but actually experience less time. The problem is the notion of two clocks' "rates". I would consider their "rates" as the ratio of the time they experience. Although I think what you mean with their rates is that a second on one, is a second on the other when they are at rest relative to eachother. You're pointing out, that the cause for the decay-experiment's result, is the time dilation between the two frames. I misunderstood you :)

Although Mitesh9 seems to have raised some questions with me..

I'd say that any frame can be considered, emphasis on considered, stationary, which is what we're doing when saying "we are in S", which you do yourself. What you can't say is that a frame "is" stationary, in some absolute sense - because of the the relativity principle.

"However, that does not mean, that, any watch has actually slowed down due to it's speed."

I don't quite know what you mean with "actually". You can't say what "actually" happens, only what happens from a certain frame. The clock's are mechanically identical, and will therefore tick at the same rate when at rest with eachother, but differently when moving relative to eachother, if the rate is considered as the ratio between the experienced time of the two clocks. I think I agree with your point though, that "clocks slow down" is a term lacking information about what you actually mean.

Although Mitesh9 seems to have raised some questions with me..

I'd say that any frame can be considered, emphasis on considered, stationary, which is what we're doing when saying "we are in S", which you do yourself. What you can't say is that a frame "is" stationary, in some absolute sense - because of the the relativity principle.

"However, that does not mean, that, any watch has actually slowed down due to it's speed."

I don't quite know what you mean with "actually". You can't say what "actually" happens, only what happens from a certain frame. The clock's are mechanically identical, and will therefore tick at the same rate when at rest with eachother, but differently when moving relative to eachother, if the rate is considered as the ratio between the experienced time of the two clocks. I think I agree with your point though, that "clocks slow down" is a term lacking information about what you actually mean.

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