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Transformation Vs. Physical Law |
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| May28-12, 11:27 AM | #18 |
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Transformation Vs. Physical LawThere is a physical law that decides the number, which law happens to be invariant under transformation . |
| May28-12, 11:41 AM | #19 |
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| May28-12, 11:44 AM | #20 |
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So your own analogy perfectly supports the facts of the Lorentz transformation; yet you talk as if you are somehow pointing out a problem. What problem? |
| May28-12, 11:48 AM | #21 |
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But what I would really like to mention is that, to refute a theory we need just one experiment where as to give a theory the stature of fundamental fact there is NO limit on the Experiments. And No, I'm not looking for paradoxes, instead I'm looking for solutions. Thanks |
| May28-12, 11:58 AM | #22 |
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| May28-12, 12:01 PM | #23 |
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| May28-12, 12:04 PM | #24 |
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| May28-12, 12:06 PM | #25 |
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That is, the number of particles reaching Earth are determined by the tools of transformation. This is a big problem, at-least to my understanding. |
| May28-12, 12:08 PM | #26 |
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Mentor
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Since it is a law of physics and since all laws of physics are diffeomorphism invariant, we know that it is invariant under the Lorentz transform. But no transform is required in order to use it. |
| May28-12, 12:09 PM | #27 |
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And this length is to be transformed. |
| May28-12, 12:17 PM | #28 |
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| May28-12, 12:20 PM | #29 |
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So there is no "length" involved--only the particles' travel time (or, if you want to be really precise, since the particles are not moving but the source and detector are, in this frame: the time between when the source is co-located with the particles and when the detector is co-located with the particles, by the particles' clock).Look at the formula DaleSpam posted, which explicitly uses the time in the particles' rest frame. Do you see any length in there? |
| May28-12, 12:21 PM | #30 |
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I was tempted to add "of course", but obviously it's not obvious or you wouldn't be asking. So here goes.... You find yourself riding a relativistic particle down from the top of the atmosphere. You see the surface of the earth rushing towards you at speed v=.999c, from a distance of 1 light-usec away. Note that neither this distance nor the speed came from any sort of transformation - you measured them directly. Now, what is the probability that your relativistic but unstable steed will hit (be hit by) the surface of the earth before it decays? Calculate the time the particle needs to live, by dividing the distance by the velocity, and plug it and lambda (the half-life of the particle expressed in terms of the particle's proper time, which is the time that you are measuring - see, still no transforms) into the formula... And out pops your answer. |
| May28-12, 12:35 PM | #31 |
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In order to pinpoint, how does one calculate when was the particle at source and when at the detector? The simple equation would have been, contracting the distance between the source and detector and dividing it by the relative velocity. But you never mentioned how are you going to calculate when the particle was at source and how much time it took to reach the detector. |
| May28-12, 12:40 PM | #32 |
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| May28-12, 12:42 PM | #33 |
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Mentor
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| May28-12, 12:54 PM | #34 |
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No it cannot, the same applies to the number of particles reaching Earth. That is, No matter what, in the end the ratio of the number of particles reaching Earth to the number of particles survived in the lab, is always a function of the speed of the particles which reach in higher quantity. What you guys are missing is the point that, we need to use that same law for lab particles also. Thanks |
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