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| Tags: dead, proof, relativity, second, special |
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#1
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There IS NO theory in which the universe appears the same, regardless
of inertial frame (considering the properties of light). S.R. is a good try, but it won't work because you will get into trouble as soon as you start accelerating. There is a twin-experiment possible with only one acceleration, namely that of the traveling clock at the far destination, to reverse speed for the back journey. As soon as the traveling clock arrives back at the stationary clock, it is discovered that the stationary clock is time T ahead instead of time T behind, contrary to what was to be expected, based upon the principles of S.R. The only cause can be the one acceleration in the journey of the traveling clock. Because only during this acceleration the conditions of S.R. were broken, it is that during this acceleration the stationary clock overtook/caught-up the time difference of no less than 2 * T, as seen from the traveling clock. However, the length of T is dependent on the length of the journey and not on the length or intensity of the acceleration. If the traveling clock were to travel ten times as far, the SAME acceleration to return would have a ten-fold overtake/catch-up as NECESSARY consequence to ensure consistence of clocks upon arrival. This weird overtake/catch-up behaviour is against symmetries in nature that are far more basic than the symmetry that is "gained" by S.R. Moreover: it is against what everyone knows of nature. The necessary overtake/catch-up behaviour can be detected! The stationary clock can send pulses at regular times by radio or light signals. They will be received by the traveling clock, obeying the rules of Doppler and S.R., as long as there is no acceleration. As soon as the traveling clock starts accelerating (decelerating/accelerating if you will) to return back, there should come in a sudden burst of clock pulses of the stationary clock. If the journey was longer, the burst will be stronger and more frantic, to catch-up the "lost" time. Every object in the neighborhood of the traveling clock, that did not this long journey, but that is subjected to the same acceleration, receives the same "burst" in clock pulses from the stationary clock. The "burst" can be arbitrarily intense, because there is no theoretical limit on the length of the journey. The universe should have if it were a "memory" for the time-loss that has to be compensated during the acceleration. Of course the universe has no such memory. S.R. leads to unacceptable consequences. We know the universe does not work this way, therefore S.R. is not a valid mathematical model for the reality of the universe. It's a pitty for mister Einstein. He is one of the biggest jokers that science has known. He has misled the world for more than 100 years (101 if I am well informed) with a fallacy that is so convoluted that everyone thought it was brilliant. However, the error can be exposed with less than 100 lines of plain english text, as shown above. What distinguishes me from all the parrots on this forum (the majority) that "believe" in S.R.? I have the courage to use my common sense and to draw conclusions. You have all been misled... unfortunately... And by sticking to theories that are impossible you make yourself immortally laughable. |
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#2
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#3
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Dear David, There are many such theories. Many of those also agree with experiment. *THE* S.R. theory has consequences that are incompatible with simple properties of observations of clock pulses under acceleration. S.R. cannot agree with all experiments is what I have shown in my introductory posting. If you have one that does not suffer from errors that can already be exposed by simple reasoning, let me know. S.R. is a good try, but it won't work because you will get into trouble as soon as you start accelerating. No. SR can be extended to make correct predictions with acceleration. SR simply does not do gravitation. You did not follow my argument. My reasoning is: if we adopt S.R. for the parts of the experiment that are not accelerated, we are left with a remaining part with acceleration that must exhibit such weird behaviour that no theory for it is immaginable. The point is that I did not assume any theory for the acceleration part, not even S.R. The thought experiment shows an accelerated part in which not even time symmetry holds. The "burst" of timing pulses you receive under acceleration is proportional to the length of your journey. This is a violation of time symmetry. The experiment gives different results, based on the history of it. You can do a twin experiment with three clocks and *no* accelerations. But the results are mutually consistent. The acceleration is only there to minimize clocks. You can have two travelling clocks, one at v+, one at v-, and have them "pass syncronization" a distance L away from your stationary clock. I know. I want you to react on my experiment and not on a concocted one that is designed to cover the flaws of S.R. By "ahead", I assume you mean that it indicates more elapsed time? If this is what you mean, then you misunderstand what relativity predicts. It predicts a shorter elapsed time for the moving clock. S.R. predicts that any moving clock walks slower than a stationary clock, as seen from the stationary clock. Agreed? I have never meant anything else. Actually your error(s) was / were exposed in much less than 100 lines. What you did expose was your inability to explain the problems that occur in MY experiment. Goodbye, Dr. J.C. Verheul. |
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#4
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wrote in message ps.com... There IS NO theory in which the universe appears the same, regardless of inertial frame (considering the properties of light). S.R. is a good try, but it won't work because you will get into trouble as soon as you start accelerating. There is a twin-experiment possible with only one acceleration, namely that of the traveling clock at the far destination, to reverse speed for the back journey. I don't understand what you mean with "only one acceleration". If there is a back journey, there must have been a forward journey. To begin the forward journey the clock K' must accelerate away from the stationnary clock K. To terminate the back journey and return to K, K' must also accelerate. So I count 3 accelerations. So in order to understand what you have exactly in mind, can you elaborate on this in terms of the following? We have two identical clocks K and K' at the same place. They show the same time 0. Can you explain in detail what happens next in your experiment? Dirk Vdm |
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#5
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Dirk,
I assume acceleration of the traveling clock before synchronizing, and deceleration after time comparison at arrival. Clocks can be synchronized at a very close passage, even when they are moving with regard to one another. So the traveling clock is first accelerated, on top speed it passes very close the stationary clock and both are synchronized. Upon arrival the inverse procedure is followed. This is an important aspect of the experiment, because if we have only one acceleration, we can "corner" the problems that S.R. leads to, which is demonstrated in my introductory posting. Regards, Jan. |
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#6
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#7
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wrote in message ups.com... Dirk, I assume acceleration of the traveling clock before synchronizing, and deceleration after time comparison at arrival. Clocks can be synchronized at a very close passage, even when they are moving with regard to one another. So the traveling clock is first accelerated, on top speed it passes very close the stationary clock and both are synchronized. Upon arrival the inverse procedure is followed. Ok. We could do the same thing at the turnaround event. At that "return point" the outbound clock's time is taken over onto a returning clock that was already accelerated on its way "back home". This way we would have no acceleration. Would that invalidate anything you said in your intro posting? Dirk Vdm |
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#8
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wrote: There IS NO theory in which the universe appears the same, regardless of inertial frame (considering the properties of light). S.R. is a good try, but it won't work because you will get into trouble as soon as you start accelerating. Can you find the word *inertial* in the first 17 chapters of this paper? http://www.bartleby.com/173/ (1920) Using Google, I got a hit at chapter 23...but that is the GR section. Sue... [...] |
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#9
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#10
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"Sue..." wrote in message ups.com... wrote: There IS NO theory in which the universe appears the same, regardless of inertial frame (considering the properties of light). S.R. is a good try, but it won't work because you will get into trouble as soon as you start accelerating. Can you find the word *inertial* in the first 17 chapters of this paper? http://www.bartleby.com/173/ (1920) "Inertial" is defined as "in which Newton's Laws apply", i.e. "in which objects continue to travel in straght lines if no external forces act on them". Using Google, I got a hit at chapter 23...but that is the GR section. You won't find something you ignore (or pretend to ignore) with Google, Dennis Dirk Vdm |
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