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| Tags: criminal, cult, einstein, sagnac |
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#11
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Dono wrote:
On May 26, 10:18 am, Tom Roberts wrote: Dono wrote: http://arxiv.org/PS_cache/gr-qc/pdf/9912/9912014v8.pdf While it is true that over a non-local distance GR predicts anisotropy in the round-trip speed of light, in practice this is too small to measure on earth. The calculations in the "paper" are still wrong, right? I have not checked them or read the paper in detail. Skipping to the end the paper says the effect is too small to measure, which is correct. Tom Roberts |
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#12
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On May 26, 6:07 pm, Tom Roberts wrote:
Dono wrote: On May 26, 10:18 am, Tom Roberts wrote: Dono wrote: http://arxiv.org/PS_cache/gr-qc/pdf/9912/9912014v8.pdf While it is true that over a non-local distance GR predicts anisotropy in the round-trip speed of light, in practice this is too small to measure on earth. The calculations in the "paper" are still wrong, right? I have not checked them or read the paper in detail. Skipping to the end the paper says the effect is too small to measure, which is correct. Tom Roberts Look at formulas (1) and (2). The guy doesn't understand closing speed, he thinks that c varies depending on direction (upward vs. downward). To make matters worse, he uses the newtonian at^2 |
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#13
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Dono wrote:
On May 26, 6:07 pm, Tom Roberts wrote: Look at formulas (1) and (2). The guy doesn't understand closing speed, he thinks that c varies depending on direction (upward vs. downward). To make matters worse, he uses the newtonian at^2 I have no interest in studying and then debating this paper. But I remark that in GR, for a non-local path [#], on the surface of the earth, the measured 1-way speed of light _is_ different up from down, for any sensible method of synchronizing clocks. Moreover, the 1-way speed of light measured with real clocks will _vary_ when measured over a non-local vertical path, with the value depending on how much time has elapsed between synchronizing the clocks and making the measurement. So it's clear that such measurements are not just measuring the 1-way speed of light (which cannot vary for such a static situation), but are also displaying limitations of the instruments. [#] By "non-local" I mean a path long enough and with clocks accurate and precise enough to detect the tiny variations I'm discussing. In practice this is negligible, even for the best available laboratory clocks. Measuring the speed of light over round-trip paths does not suffer from this problem, and over non-local paths is anisotropic on the surface of the earth. But in practice the magnitude of this anisotropy is well below measurement resolutions. Tom Roberts |
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#14
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On May 26, 10:15 pm, Dono wrote:
On May 26, 6:07 pm, Tom Roberts wrote: Dono wrote: On May 26, 10:18 am, Tom Roberts wrote: Dono wrote: http://arxiv.org/PS_cache/gr-qc/pdf/9912/9912014v8.pdf While it is true that over a non-local distance GR predicts anisotropy in the round-trip speed of light, in practice this is too small to measure on earth. The calculations in the "paper" are still wrong, right? I have not checked them or read the paper in detail. Skipping to the end the paper says the effect is too small to measure, which is correct. Tom Roberts Look at formulas (1) and (2). The guy doesn't understand closing speed, he thinks that c varies depending on direction (upward vs. downward). To make matters worse, he uses the newtonian at^2 Tom Roberts is consistant in perfering a causality violating interpretation of Pound-Rebka rather than the Pound-Snider nuclear resonance interpretation as Okun suggest: The classical phenomenon of the redshift of light in a static gravitational potential, usually called the gravitational redshift, is described in the literature essentially in two ways: on the one hand the phenomenon is explained through the behaviour of clocks which run the faster the higher they are located in the potential, whereas the energy and frequency of the propagating photon do not change with height. The light thus appears to be redshifted relative to the frequency of the clock. On the other hand the phenomenon is alternatively discussed (even in some authoritative texts) in terms of an energy loss of a photon as it overcomes the gravitational attraction of the massive body. This second approach operates with notions such as the "gravitational mass" or the "potential energy" of a photon and we assert that it is misleading. We do not claim to present any original ideas or to give a comprehensive review of the subject, our goal being essentially a pedagogical one. http://arxiv.org/abs/physics/9907017 Taking the 3-space length of a 4-space world line is necessary to make the twins age absrudly so don't expect Tom to find the faults that you do in the paper and give up his "magic trick" Sue... |
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#15
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Dono wrote: On May 26, 9:20 am, Pentcho Valev wrote: Androcles wrote in sci.physics.relativity: "ca314159" wrote in ... The Michelson-Morley experiment assumes that the "source" of the light in the interferometer can be wholely represented in only one frame of reference, the lab frame (where the null result occurs). The source of light in the Michelson-Morley experiment must be represented by two separate frames: The leg of the interferometer where radiation was expected to be affected by its relative motion with respect to an aether, composes one frame of reference. I will call this the lab frame. The other leg of the interferometer composed a completely different frame of reference; effectively, it was not in relative motion with respect to the aether; in this leg there was no expected influence of an aether wind upon the radiation and so it can be considered as a separate frame from the lab frame and treated as if it were being dragged along with the aether. I will call this the aether frame. But the actual light source of the Michelson-Morley experiment effectively exists at the intersection of these two different frames of reference and yet emits the same radiation into both of them; so then, how can we say that the source will be affected by the relative motion between the lab frame and the aether frames when the light source exists inside both frames at the same time? We can't, and that's why there's a null result. You can theorise all you want to, Sagnac doesn't get a null result but it would if you stopped it turning. http://www.androcles01.pwp.blueyonde...nac/Sagnac.htm Sagnac's experiment can be regarded as a proof that Einstein criminal cult has managed to destroy rationality in science completely. There can be no other experiment more convincingly refuting Einstein's false principle of constancy of the speed of light and yet simple and even naive camouflage devised by Einstein criminal cult has been absolutely efficient for almost a century: http://arxiv.org/PS_cache/gr-qc/pdf/9909/9909081v7.pdf Propagation of light in non-inertial reference frames Vesselin Petkov Science College, Concordia University 1455 De Maisonneuve Boulevard West Montreal, Quebec, Canada H3G 1M8 "The Sagnac effect can de described as follows. Two light signals emitted from a point M on the rim of a rotating disk and propagating along its rim in opposite directions will not arrive simultaneously at M. There still exist people who question special relativity and their main argument has been this effect. They claim that for an observer on the rotating disk the speed of light is not constant - that the Galilean law of velocity addition (c+v and c v, where v is the orbital speed at a point on the disk rim) should be used by the rotating observer in order to explain the time difference in the arrival of the two light signals at M. What makes such claims even more persistent is the lack of a clear position on the issue of the speed of light in non- inertial reference frames. What special relativity states is that the speed of light is constant only in inertial reference frames - this constancy follows from the impossibility to detect absolute motion (more precisely, it follows from the non-existence of absolute motion). Accelerated motion can be detected and for this reason the coordinate velocity of light in non-inertial reference frames is a function of the proper acceleration of the frame. The rotating disk is a non-inertial reference frame and its acceleration can be detected by different means including light signals. That is why it is not surprising that the coordinate velocity of light as determined on the disk depends on the centripetal acceleration of the disk." Pentcho Valev Now it is clear where you get all your ideas. Check this out, by the same "scientist": http://arxiv.org/PS_cache/gr-qc/pdf/9810/9810030v14.pdf The idiot apparently never heard of Pound-Rebka. You believe other relativists are cleverer? Besides, Vesselin Petkov is not an ordinary relativist - he is one of the leaders of the so- called Minkowski spacetime money-makers - an influential cartel in Einstein criminal cult: http://www.spacetimesociety.org/ http://www.spacetimesociety.org/conferences/2008/ Pentcho Valev |
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#16
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On May 26, 9:13 pm, Tom Roberts wrote:
Dono wrote: On May 26, 6:07 pm, Tom Roberts wrote: Look at formulas (1) and (2). The guy doesn't understand closing speed, he thinks that c varies depending on direction (upward vs. downward). To make matters worse, he uses the newtonian at^2 I have no interest in studying and then debating this paper. But I remark that in GR, for a non-local path [#], on the surface of the earth, the measured 1-way speed of light _is_ different up from down, for any sensible method of synchronizing clocks. Moreover, the 1-way speed of light measured with real clocks will _vary_ when measured over a non-local vertical path, with the value depending on how much time has elapsed between synchronizing the clocks and making the measurement. So it's clear that such measurements are not just measuring the 1-way speed of light (which cannot vary for such a static situation), but are also displaying limitations of the instruments. [#] By "non-local" I mean a path long enough and with clocks accurate and precise enough to detect the tiny variations I'm discussing. In practice this is negligible, even for the best available laboratory clocks. Measuring the speed of light over round-trip paths does not suffer from this problem, and over non-local paths is anisotropic on the surface of the earth. But in practice the magnitude of this anisotropy is well below measurement resolutions. Tom Roberts This is interesting, much more interesting than all the crackpot stuff that started the discussion. Is the proof easy to derive? Can you do a short writeup? (the math associated with it would be great). |
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#17
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Pentcho Valev wrote: Tom Roberts wrote: Pentcho Valev wrote: Sagnac's experiment can be regarded as a proof that Einstein criminal cult has managed to destroy rationality in science completely. There can be no other experiment more convincingly refuting Einstein's false principle of constancy of the speed of light This is plain and simply not true. The constancy of the speed of light in SR applies ONLY to inertial frames. The rotating Sagnac apparatus is manifestly not inertial. Indeed, applying an SR analysis in the inertial frame of its center one obtains values that agree with experimental observations. References Roberts Roberts? (If possible available on the internet) Exercise for the reader: show QUANTITATIVELY that for a Sagnac apparatus on the surface of the earth the effects of gravitation and earth's rotation and revolution are all negligible. Valev continually and repeatedly tries to discuss things he does not understand, and makes numerous errors therein. And his stupid writing style underscores his lack of knowledge. He needs to grow up and STUDY, rather than wasting time posting nonsense to the net. I do not have time right now Roberts Roberts but tomorrow I am going to compare my stupidity and your stupidity: http://groups.google.com/group/sci.p...c45cb1c4adda7? Tom Roberts in sci.physics.relativity: "The speed of the light is also independent of source velocity, both in SR and GR, and experimentally. The frequency and wavelength of the emitted light, however, are not independent of source velocity, and depend upon the relative velocity of the source and observer, including the direction of this velocity 3- vector wrt the beam of light. The SR Doppler formula describes this quite well (i.e. agrees with experimental measurements)." Tom Roberts Roberts Roberts your silence prevents me from comparing my stupidity and your stupidity. Just answer a simple question Roberts Roberts: Would you call the distance between two consecutive flashes emitted by a light source "wavelength"? See more in http://groups.google.com/group/sci.p...2830d9a42e1c1? Pentcho Valev |
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#18
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On May 26, 8:10 pm, "Androcles" wrote:
The word "inertial" appears nowhere in "On the Electrodynamics of Moving Bodies". What special relativity DOES claim is contained in the last three paragraphs of section 4, which clearly refers to non-inertial frames. http://www.fourmilab.ch/etexts/einstein/specrel/www/ "Thence we conclude that a balance-clock at the equator must go more slowly, by a very small amount, than a precisely similar clock situated at one of the poles under otherwise identical conditions." But instead of inertial he writes 'uniform translatory motion'. And if you had quoted all the relevant part, everyone would have seen that Einstein was assuming that motion along a curve could be analyzed as a composite inertial motion, which I assume was only temptative at this time when he had not yet developed GR. Here is the missing part of your quotation: "If we assume that the result proved for a polygonal line is also valid for a continuously curved line, we arrive at this result: If one of two synchronous clocks at A is moved in a closed curve with constant velocity until it returns to A, the journey lasting t seconds, then by the clock which has remained at rest the travelled clock on its arrival at A will be second slow". Best regards |
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#19
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"LauLuna" wrote in message oups.com... : On May 26, 8:10 pm, "Androcles" wrote: : : : The word "inertial" appears nowhere in "On the Electrodynamics of Moving : Bodies". : What special relativity DOES claim is contained in the last three paragraphs : of section 4, : which clearly refers to non-inertial frames. : http://www.fourmilab.ch/etexts/einstein/specrel/www/ : : "Thence we conclude that a balance-clock at the equator must go more slowly, : by a very small amount, than a precisely similar clock situated at one of : the poles under otherwise identical conditions." : : : But instead of inertial he writes 'uniform translatory motion'. : I'm not so deranged that I hallucinate a clock at the equator is in 'uniform translatory motion'. : And if you had quoted all the relevant part I did, imbecile. The relevant part is where the great astrologer Einstein applies his crystal ball readings and palmistry to the real Earth, dolt. I'll decide what's relevant, idiot. : , everyone would have seen 'Everyone' can read for themselves, some of them can even think for themselves. : that Einstein was assuming Yes, you have that right. Congratulations, genius, take one brownie point. Einstein does a lot of assuming and no proving. That's how the fine art of persuading the gullible is accomplished. : that motion along a curve could be analyzed : as a composite inertial motion, which I assume *You* assume? Einstein does all the assuming for you, cretin. Ass-u-me makes an ass out of u and ewe, not u and me. "Thence we CONCLUDE" that Einstein didn't realise atomic clocks would someday disprove his quack crackpottery. : was only temptative at : this time when he had not yet developed GR. Here is the missing part : of your quotation: : : "If we assume that the result proved for a polygonal line is also : valid for a continuously curved line, we arrive at this result: If one : of two synchronous clocks at A is moved in a closed curve with : constant velocity until it returns to A, the journey lasting t : seconds, then by the clock which has remained at rest the travelled : clock on its arrival at A will be second slow". : Here is the missing part of *your* quotation: "1/2 tv^2/c^2". Here is the missing part of your brain, plug it in and think clearly: "If we assume that the result proved for a polygonal line is also valid for a continuously curved line, we arrive at this result: If one of two synchronous sundials at A is moved in a closed curve with constant velocity until it returns to A, the journey lasting t seconds, then by the sundial which has remained at rest the travelled sundial on its arrival at A will be 1/2 tv^2/c^2 millenia slow". I do not assume that the result proved for a polygonal line was proved at all. In fact it was disproved by Einstein himself in section 3, which you *might* see clearly by making the polygon a square. http://www.fourmilab.ch/etexts/einst...ures/img26.gif Now all you need do is apply the Anderson transformations. "That is, we can reverse the directions of the frames which is the same as interchanging the frames, which - as I have told you a LOT of times, OBVIOUSLY will lead to the transform: t = (tau-xi*v/c^2)/sqrt(1-v^2/c^2) x = (xi - v*tau)/sqrt(1-v^2/c^2) or: tau = (t+xv/c^2)/sqrt(1-v^2/c^2) xi = (x + vt)/sqrt(1-v^2/c^2)" -Paul B. Andersen : Best regards Thank you. Without regards, Androcles. |
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#20
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Dono wrote:
On May 26, 9:13 pm, Tom Roberts wrote: But I remark that in GR, for a non-local path [#], on the surface of the earth, the measured 1-way speed of light _is_ different up from down, for any sensible method of synchronizing clocks. [...] This is interesting, much more interesting than all the crackpot stuff that started the discussion. Is the proof easy to derive? Can you do a short writeup? (the math associated with it would be great). Already posted to this newsgroup, long ago (1998): http://groups.google.com/group/sci.p...2?dmode=source (I of course applied the equivalence principle to convert the conclusions of this SR computation to the earth's surface.) That is a computation in SR, in GR one would integrate the metric over the light path. That's more complicated, but for the Schwarzschild manifold and vertical paths it can be done. Somewhere I have a Mathematica notebook with this computation for LIGO detecting sun and moon (unfortunately they have no sensitivity at all for signals of this frequency). The conclusions are essentially the same, but the details differ a bit.... Tom Roberts |
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