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#1
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"What Broke the Symmetry?"
All of the below is based solely on Einstein's "Train/Embankment" Gedanken: (see http://www.bartleby.com/173/9.html) Given: Two events E(1) and E(2) occur as inertial observers A and B meet between the events. E(1)---------------------------------------------E(2) ---light ray----------------------- light ray--- ------------------------A------------------------- ------------------------B------------------------- As shown, observers A and B are now symmetrical with respect to the events. However, as Einstein stated, the observers will see the light rays arrive _differently_, so the initial symmetry becomes broken. This brings us to today's critical query, namely, **********What breaks the symmetry?********** We can answer this important question by using the simple process of elimination, as follows: There are only three things involved here, viz., (i) events, (ii) light rays, and (iii) observers. it goes without saying that the events did not break the symmetry, so this leaves only light rays and the observers; since the light rays merely mimic the events, we see that they are also innocent; this leaves only the observers. But what is it about the observers that broke the symmetry? As Einstein said, they moved __differently__ with respect to the light rays. Paraphrasing Einstein: "Although the embankment observer sees the light beams arrive simultaneously, the train observer is hastening towards one beam of light, whilst he is riding on ahead of the other beam of light, so he does not see the beams arrive simultaneously; specifically, he will see the beam toward which he is moving __before__ he sees the beam from which he is moving." AN IMPORTANT CONCLUSION: Clearly, Einstein's Gedanken proves that inertial observers in different frames move __differently__ with respect to any given light ray. AN IMPORTANT COROLLARY: If inertial observers A and B move __differently__ relative to a light ray, then the ray must in turn move __differently__ relative to the observers; this means that light's speed relative to the observers __differs__. ANOTHER IMPORTANT COROLLARY: Clock pairs in various inertial frames cannot be started simultaneously by light rays which are emitted by a midway source, so the clocks of special relativity cannot be synchronous (except for those in the few frames which remain symmetrical about the source). YET ANOTHER IMPORTANT COROLLARY: Given relativity's asynchronous clocks, light's speed cannot be accurately determined. THE FINAL IMPORTANT COROLLARY: Given synchronous clocks, light's speed __can__ be accurately determined, and, as we know, it will then vary with frame velocity. |DE| -- Posted via a free Usenet account from http://www.teranews.com |
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#2
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"Dark Energy" wrote in message ... "What Broke the Symmetry?" All of the below is based solely on Einstein's "Train/Embankment" Gedanken: (see http://www.bartleby.com/173/9.html) Given: Two events E(1) and E(2) occur as inertial observers A and B meet between the events. E(1)---------------------------------------------E(2) ---light ray----------------------- light ray--- ------------------------A------------------------- ------------------------B------------------------- As shown, observers A and B are now symmetrical with respect to the events. If, according to A, the events are simultaneous and equidistant, then, according to B, they are not simultaneous and not equidistant, and vice versa. You can have symmetry between A and B, if the events are simultaneous and equidistant according to some third observer C, w.r.t. whom A and B move with the same speed in opposite directions. Does this help? Dirk Vdm |
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#3
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Dark Energy wrote: "What Broke the Symmetry?" All of the below is based solely on Einstein's "Train/Embankment" Gedanken: (see http://www.bartleby.com/173/9.html) Given: Two events E(1) and E(2) occur as inertial observers A and B meet between the events. E(1)---------------------------------------------E(2) ---light ray----------------------- light ray--- ------------------------A------------------------- ------------------------B------------------------- As shown, observers A and B are now symmetrical with respect to the events. However, as Einstein stated, the observers will see the light rays arrive _differently_, so the initial symmetry becomes broken. This brings us to today's critical query, namely, **********What breaks the symmetry?********** We can answer this important question by using the simple process of elimination, as follows: There are only three things involved here, viz., (i) events, (ii) light rays, and (iii) observers. it goes without saying that the events did not break the symmetry, so this leaves only light rays and the observers; since the light rays merely mimic the events, we see that they are also innocent; this leaves only the observers. Sorry... there are only three things *considered*. There are more than three things *involved* and they are left ambiguous. That make the illustration invalid as any kind of useful thought experiment. Propagation in a dielectric medium http://farside.ph.utexas.edu/teachin...es/node98.html http://en.wikipedia.org/wiki/Wave_impedance http://en.wikipedia.org/wiki/Free_space http://www-ssg.sr.unh.edu/ism/what.html Abstract Einstein addressed the twin paradox in special relativity in a relatively unknown, unusual and rarely cited paper written in 1918, in the form of a dialogue between a critic and a relativist. Contrary to most textbook versions of the resolution, Einstein admitted that the special relativistic time dilation was symmetric for the twins, and he had to invoke, asymmetrically, the general relativistic gravitational time dilation during the brief periods of acceleration to justify the asymmetrical aging. Notably, Einstein did not use any argument related to simultaneity or Doppler shift in his analysis. I discuss Einstein's resolution and several conceptual issues that arise. It is concluded that Einstein's resolution using gravitational time dilation suffers from logical and physical flaws, and gives incorrect answers in a general setting. The counter examples imply the need to reconsider many issues related to the comparison of transported clocks. The failure of the accepted views and resolutions is traced to the fact that the special relativity principle formulated originally for physics in empty space is not valid in the matter-filled universe. C. S. Unnikrishnan Gravitation Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400 005, India http://www.iisc.ernet.in/currsci/dec252005/2009.pdf "The [ ] Incompatibility of the Law of Propagation of Light with the Principle of Relativity [is only] Apparent" http://www.bartleby.com/173/7.html Time-independent Maxwell equations Time-dependent Maxwell's equations http://farside.ph.utexas.edu/teachin.../lectures.html Maxwell's equations in classic electrodynamics (classic field theory)_ a) Maxwell equations (no movement), b) Maxwell equations (with moved bodies) http://www.wolfram-stanek.de/maxwell...assic_extended But what is it about the observers that broke the symmetry? As Einstein said, they moved __differently__ with respect to the light rays. Paraphrasing Einstein: "Although the embankment observer sees the light beams arrive simultaneously, the train observer is hastening towards one beam of light, whilst he is riding on ahead of the other beam of light, so he does not see the beams arrive simultaneously; specifically, he will see the beam toward which he is moving __before__ he sees the beam from which he is moving." AN IMPORTANT CONCLUSION: Clearly, Einstein's Gedanken proves that inertial observers in different frames move __differently__ with respect to any given light ray. Frayed knot: A Lorentz transformation or any other coordinate transformation will convert electric or magnetic fields into mixtures of electric and magnetic fields, but no transformation mixes them with the gravitational field. http://www.aip.org/pt/vol-58/iss-11/p31.html Sue... AN IMPORTANT COROLLARY: If inertial observers A and B move __differently__ relative to a light ray, then the ray must in turn move __differently__ relative to the observers; this means that light's speed relative to the observers __differs__. ANOTHER IMPORTANT COROLLARY: Clock pairs in various inertial frames cannot be started simultaneously by light rays which are emitted by a midway source, so the clocks of special relativity cannot be synchronous (except for those in the few frames which remain symmetrical about the source). YET ANOTHER IMPORTANT COROLLARY: Given relativity's asynchronous clocks, light's speed cannot be accurately determined. THE FINAL IMPORTANT COROLLARY: Given synchronous clocks, light's speed __can__ be accurately determined, and, as we know, it will then vary with frame velocity. |DE| -- Posted via a free Usenet account from http://www.teranews.com |
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#4
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"Sue..." wrote in message oups.com... [...] Hey Dennis! I've never seen an aether, have you? http://tinyurl.com/yndvwx http://www.quackwatch.org/01Quackery...cs/pseudo.html http://www.youtube.com/watch?v=Pf3z935R37E |
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#5
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Dirk Van de moortel wrote:
Does this help? Yes, it helped to confuse the issue. You need to read the following from Einstein: "If an observer sitting in the position M' in the train did not possess this velocity, then he would remain permanently at M, and the light rays emitted by the flashes of lightning A and B would reach him simultaneously, i.e. they would meet just where he is situated." As I said, and as Einstein said, the only reason the observers saw the light beams arrive differently was the observers' different velocities wrt to the light beams. |DE| -- Posted via a free Usenet account from http://www.teranews.com |
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#6
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"Dark Energy" wrote in message ... Dirk Van de moortel wrote: Does this help? Yes, it helped to confuse the issue. I thought it wouldn't help, but it could have been worth the try. Dirk Vdm |
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#7
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Dark Energy wrote: "What Broke the Symmetry?" All of the below is based solely on Einstein's "Train/Embankment" Gedanken: (see http://www.bartleby.com/173/9.html) Given: Two events E(1) and E(2) occur as inertial observers A and B meet between the events. E(1)---------------------------------------------E(2) ---light ray----------------------- light ray--- ------------------------A------------------------- ------------------------B------------------------- As shown, observers A and B are now symmetrical with respect to the events. As viewed from which frame? Paul Cardinale |
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#8
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Paul Cardinale wrote:
Dark Energy wrote: E(1)---------------------------------------------E(2) ---light ray----------------------- light ray--- ------------------------A------------------------- ------------------------B------------------------- As shown, observers A and B are now symmetrical with respect to the events. As viewed from which frame? Paul Cardinale From any frame. As Einstein said, at the time of the above diagram, "If an observer sitting in the position M' in the train did not possess this velocity, then he would remain permanently at M, and the light rays emitted by the flashes of lightning A and B would reach him simultaneously, i.e. they would meet just where he is situated." In other words, at the time of the above diagram, M and M' are interchangeable and equivalent, so they are symmetrical wrt the events and to the light rays coming from them. Perhaps I should not have taken it for granted that most folk here understood Einstein's famous Train/Embankment Gedanken. |DE| -- Posted via a free Usenet account from http://www.teranews.com |
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#9
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"Dark Energy" wrote in message ... Paul Cardinale wrote: Dark Energy wrote: E(1)---------------------------------------------E(2) ---light ray----------------------- light ray--- ------------------------A------------------------- ------------------------B------------------------- As shown, observers A and B are now symmetrical with respect to the events. As viewed from which frame? Paul Cardinale From any frame. As Einstein said, at the time of the above diagram, "If an observer sitting in the position M' in the train did not possess this velocity, then he would remain permanently at M, and the light rays emitted by the flashes of lightning A and B would reach him simultaneously, i.e. they would meet just where he is situated." In other words, at the time of the above diagram, M and M' are interchangeable and equivalent, so they are symmetrical wrt the events and to the light rays coming from them. Perhaps I should not have taken it for granted that most folk here understood Einstein's famous Train/Embankment Gedanken. Perhaps you should ask questions and find out where exactly your brain gets stuck, as opposed to making a fool of yourself by trying to prove that the rest of the planet is populated with idiots. Dirk Vdm |
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#10
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On Thu, 18 Jan 2007 20:54:48 GMT, "Dirk Van de moortel"
wrote: Perhaps you should ask questions and find out where exactly your brain gets stuck, as opposed to making a fool of yourself by trying to prove that the rest of the planet is populated with idiots. Maybe you have something there. Here's my question: How do M and M' differ at the start of Einstein's Train/Embankment Gedanken? |DE| -- Posted via a free Usenet account from http://www.teranews.com |
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