See my correction: the footnote was not by Einstein. Einstein made his prediction only for a balance clock, for the reason that Sommerfeld(?) explained and which I elaborated here - the clock prediction is not valid for a partial clock. You can check the original footnotes through the link in the German Wikipedia. http://users.physik.fu-berlin.de/~kleinert/files/1905_17_891-921.pdfchoran said:Hmm, interesting: I just read that Sommerfield added the "pendulum clock" language in a 1913 edit/reissuance of the paper, and that Einstein's original words had been "balance clock". [..].
The prediction is valid as I stated in post 31. Thus in principle a pure SR test with transporting clocks is possible; but I don't know if anyone ever bothered. All such tests that I know about involved both velocity and height changes, and the GR prediction includes the SR prediction.choran said:[..] I wonder then how the theory can be tested in an Earth (or near earth) setting, since (I think) that even atomic clocks vary not just according to velocity, but by altitude above the earth. I'm just saying that this makes the theory (SR, not GR) one that may be impossible for us to test. [..].
Only atomic clock tests that I know of. Once more, check out the other experiments - there are several mentioned that you overlooked. http://math.ucr.edu/home/baez/physics/Relativity/SR/experiments.html#Tests_of_time_dilationchoran said:Thanks Harrylin, I greatly appreciate your responses, and I understand what you're saying. I agree (if this is your position, not trying to put words in your mouth) that all tests normally referred to have been tests of GR. I also agree that a pure SR test has not been done. I don't know enough to agree or disagree that the "GR prediction includes the SR prediction", or whether a straight SR test could be done. Just don't know on that one. Thanks again for your answers. You have certainly mastered a very difficult subject matter.
Yes, you are wrong. Please read the sticky on experimental tests of SR. First, it is wrong that all tests of SR have involved terrestrial sources. Second, it is wrong that SR is impossible to test, it is emminently falsifiable. There are many possible tests of SR regardless of the fact that the Earth has gravity.choran said:I'm just saying that this makes the theory (SR, not GR) one that may be impossible for us to test. All of the tests at this point (again, SR, not GR) have of necessity involved tests on or near the earth, and I know of no clock we could use to satisfy the definition of a good clock. Maybe I'm wrong.
To emphasize what The_Duck says here, in a typical particle accelerator the particles travel in a horizontal path, so there is no difference in gravitational potential and therefore no gravitational time dilation, even according to GR. This is just one example of a test that is carried out in a gravitational field that is nonetheless a test of SR. The sticky is full of others.The_Duck said:There are plenty of examples of time dilation in which only the special relativistic time dilation due to speed matters. For example you can look at the lifetime of muons in particle accelerators. These muons are going very fast and so their lifetime is extended due to time dilation. This is a purely special relativistic effect and general relativity is not needed to explain it.
tzadduki said:I have made a mistake in the first post. By time dilation we have t2-t1 > t'2-t'1 and so for light beam traveling in the x-axis direction both the numerator and denominator in S' decrease by same factor thereby making C'=C. But for the light beam traveling in the y-axis direction we will have C'>C and so the problem remains as SR says C' should be equal to C in ALL directions! thanks.
choran said:Could you post a link the the article, assuming it available online? Thank you.
tzadduki said:I have found an article where the author says the following about einstein's SR: If we have two reference frames, S and S', with S stationary and the S' moving along the 'x' axis with speed 'v' of S, then as per SR there is length contraction in the 'x' direction but no change in the 'y' or the 'z' directions of objects in S'. That is y=y' and z=z'. If we take just the y=y', then the length y2-y1 = y'2-y'1. However, SR says that the time is slower in S' than in S. This means t2-t1 is < t'2-t'1. So, if we have a beam of light traveling along the y-axis in S then the speed of the light is C= y2-y1/t2-t1. For the observer in S' who is also looking at the same beam of light it will be C'= y'2-y'1/t'2-t'1. Now, the numerators are equal but the denominator in S' is larger than in S due to time dilation. This means C'<C, which contradicts the constancy of the speed of light postulate of SR! Also, for light traveling in x-axis direction we have from length contraction x2-x1 > x'2-x'1 and from time dilation we have t2-t1 < t'2-t'1, then the speed of light in S is C=x2-x1/t2-t1 and in S' it is C'= x'2-x'1/t'2-t'1. So, for C' we have the numerator that is smaller than in S and the denominator that is greater than that in S. This again leads to C' < C !. So, how do we resolve this? thanks.
yuiop said:I think you are incorrectly assuming that the light will be traveling along the y-axis in both both S and S'. If it is traveling along the y-axis in S, then it will be traveling along a diagonal path in S'. You need use the resultant path length in S' taking the both the horizontal and vertical motion. Do a search for light clock to see what I mean.
Nugatory said:Either you've misunderstood the article or it's wrong.
A beam of light traveling along the y-axis in one frame is not traveling along the y-axis in the other frame - it has an x-axis component as well, and therefore travels a longer distance. The time dilation and length contraction is exactly enough to balance that effect, keep the speed of light the same.
Although a beam of light traveling along the x-axis in one frame is also traveling along the x-axis in the other frame, the distance covered from the origin of one frame as viewed from the other is different in the two frames. Again, length contraction and time dilation together exactly balance that effect.
You can see this for yourself if you choose either reference frame, imagine two pulses of light leaving the origin of that frame at time zero. After one second, the (x,y,t) coordinates of the pulse directed along the y-axis will be (0,1,1) and the coordinates of the pulse directed along the x-axis will be (1,0,1). Use the Lorentz transforms (not the contraction and dilation formulas!) to convert these into coordinates in the other frame, then calculate the distance covered by the light in one second in that frame. It'll come out to be c.
Mentz114 said:Referring to post#51. The article is not published in a peer-reviewed scientific journal. A quick reading leads me to conclude that it would not be accepted.
The author has some misunderstanding of the difference between coordinate effects and invariants.
tzadduki said:The x which is equal to +vt, where t is the time in S, will be canceled out by the movement of S' with respect to S by -vt where again t is the time in S, thereby resulting in the light traveling straight along y' with respect to the person in S', even though it is diagonal for a person in S looking at the beam in S'. This has to be the case according to the principle of relativity.
The article referenced is not from an acceptable source, which is not surprising given how eggregiously flawed the reasoning is. You cannot use the time dilation formula for light since there is no frame in which it is at rest, nor can you use the length contraction formula for the same reason. You must use the full Lorentz transform which includes all effects including length contraction, time dilation, relativity of simultaneity, abberation, Doppler, etc.tzadduki said:I have found an article where the author says the following about einstein's SR: If we have two reference frames, S and S', with S stationary and the S' moving along the 'x' axis with speed 'v' of S, then as per SR there is length contraction in the 'x' direction but no change in the 'y' or the 'z' directions of objects in S'. That is y=y' and z=z'. If we take just the y=y', then the length y2-y1 = y'2-y'1. However, SR says that the time is slower in S' than in S. This means t2-t1 is < t'2-t'1. So, if we have a beam of light traveling along the y-axis in S then the speed of the light is C= y2-y1/t2-t1. For the observer in S' who is also looking at the same beam of light it will be C'= y'2-y'1/t'2-t'1. Now, the numerators are equal but the denominator in S' is larger than in S due to time dilation. This means C'<C, which contradicts the constancy of the speed of light postulate of SR!