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| Tags: addition, evidence, experimental, srs, velocity |
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#21
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"Mitchell Jones" wrote in message ... In article , "Franz Heymann" wrote: "Mitchell Jones" wrote in message ... In article , "Franz Heymann" wrote: "Mitchell Jones" wrote in message ... In article , "Franz Heymann" wrote: [snip] I was quite precisely specific. If you do not understand what I wrote, the fault lies with your powers of comprehension. Franz ***{He understands that you are refusing to do a specific calculation comparing the relativistic and non-relativistic velocity additions, and he assumes, quite reasonably in my opinion, that your reticence is due to fear that you will get yourself into hot water. I have told him how to do it. If he is unable to do so, he should not be posting on the topic. ***{You claimed that the decay of a pion into a muon and a neutrino produced results that could be correctly calculated only by means of relativistic velocity additions. He said, in effect, "Prove it." To which you replied that, in essence, it is he, and not you, who has the burden of proving your claim. The question is, what's wrong with this picture? :-) --MJ}*** What is qwrong with your picture is the fact that you do not understand that I told him how to do the calculation. If he does not know enough kinematics to do this simple problem for himself, he should not be posting nonsense on the topic. ***{That is laughable. It was you who posted a claim on this topic. He merely asked you to back up your claim. The subject here is Franz Heymann's claim and whether he can defend it, not whether Vertner Vergon can do the standard relativistic velocity addition calculations which are explained in detail in thousands of textbooks. Stop playing silly buggers. I actually gave him the complete details of how to do the calculation. All he had to do was to do it. The question is, why you are struggling so mightily to escape the burden of proving your assertion? I am not struggling at all. I gave him complete details of how to do the calculation. If he, and you, are not able to actually do it, hard luck on both of you. The likely answer is that you were shocked to notice, after having already shot off your mouth on this subject, that if you applied standard relativistic velocity addition calculations to a pion decay, that in itself would do nothing to support your claim. Balls. Having reconstructed large numbers of pion and Kaon decays in my life, and having told Vergon how to do the job he wanted done, I have plenty to support my claim. Why not? Simple: you did not claim merely that applying the standard relativistic calculation would give an answer, but that the answer in question would be the CORRECT answer. Hence to defend your claim, you would have to do the following: (1) Describe a concrete example of a pion decay into a muon and a neutrino FOR WHICH THE RESULT OF A VELOCITY ADDITION HAS ACTUALLY BEEN MEASURED. (2) Show, by a concrete calculation, that the relativistic velocity addition formulas give an answer WHICH MATCHES WHAT WAS ACTUALLY MEASURED. (3) Show, by a concrete calculation, that the non-relativistic velocity addition formulas give an answer WHICH DOES NOT MATCH WHAT WAS ACTUALLY MEASURED. That was precisely what I told Vergon to do. I also told him that the non-relativistic reconstruction would fail to conserve momentum and energy, whereas that is *not* the case for a relativistic reconstruction. For those who wonder why the burden of proof assumed by Franz may pose a problem for him, I have no problem. It is you and Vergon who have problems in actually executing the calculations, th principles of which gave in great detail. the answer is that a method of calculating a physical result becomes accepted only after it has been tested against measurements in a number of critical cases, and has passed those tests. Yes. In the test cases, the result of the calculation is compared to actual measurements. But after the formula has been accepted, it is then used to calculate results in thousands of concrete cases for which there are no measured results. That, indeed, is the major benefit of the formula: once it has been thoroughly tested and accepted, it relieves its users of the necessity to keep doing measurements, over and over and over again, in tens of thousands of workaday cases. You are repeating yourself. It nauseates. And therein lies the rub, as far as Franz is concerned: by claiming that pion decay data prove the validity of the relativistic velocity addition formulae, he has implicitly claimed that pion decays have the characteristic of test cases--which means: they involve actual measurements of the parameters which the velocity addition formulas calculate. And that, of course, is far from a trivial claim. No. I told Vergon how to do the calculations both non-relativistically and relativistically. I told him that he would find that a non-relativistic reconstruction would not conserve energy and momentum, whereas the relativistic reconstruction does. My own attitude toward this stuff is simple: That neceaasrily has to be so, considering your level of stupidity. I seldom argue against generally accepted physics formulae, whether in the area of relativity or elsewhere. The reason is that they have for the most part been verified to good accuracy by the consideration of test cases. Thus my objections to such formulae, if any, tend to lie in the area of *interpretation* rather than in denial that they produce correct answers. For example, when I first pointed out in this group, years ago, that particle accelerators could not test the claim that no material object could exceed lightspeed, because the pushing forces used in accelerators themselves moved at the speed of light, You are an ignorant fool. The particles have to match the *phase velocity* of the accelerating field. It is dead easy to make EM fields propagate with phase velocities greater than c. It is only the group velocity which has an upper limit. there was no implication that the relativistic velocity addition formulae did not correctly predict accelerator results. The implication, instead, was that the interpretations of those formulae were in many ways incorrect. It was a crass implication which flies in the face of one hell of a lot of experimental evidence. I have also already indicated that in both linear accelerators and circular accelerators it is easy to show that it is impossible to get the particles to move faster than c. As to whether Franz is correct in thinking pion decays have the characteristics of test cases, where the velocity addition formulae are concerned, I had no opinion when he made his original assertion. It is utterly irrelevant whether or not you have an opinion on any matter concerning physics. However, his subsequent attempts to escape the burden of backing up his claim have made me increasingly suspicious that he is, as usual, just blowing smoke. I have not tried to escape any burden. I have given the details of how to do the calculations of which I spoke. If you and Vergon are too stupid to actually get down to doing it, that is your problem Now bugger off. Franz |
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#22
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In article ,
"Franz Heymann" wrote: Stop playing silly buggers. Balls. That neceaasrily has to be so, considering your level of stupidity. You are an ignorant fool. It was a crass implication which flies in the face of one hell of a lot of experimental evidence. It is utterly irrelevant whether or not you have an opinion on any matter concerning physics. If you and Vergon are too stupid to actually get down to doing it, that is your problem Now bugger off. ***{I'll be happy to, Franz, but first one of the following conditions must be met: (1) I'll have to be convinced that you are not an ignorant, arrogant, pretentious asshole. (2) I'll have to be convinced that you are not stupid and intellectually dishonest. (3) I'll have to be convinced that you would rather deal with me than be chain-dragged across the Arizona desert. (4) I'll have to be damn good and ready. Since (1) through (3) will not happen while the sun yet shines, I guess you'll just have to wait for (4). :-) --Mitchell Jones}*** Franz |
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#23
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"Mitchell Jones" wrote in message ... In article , "Franz Heymann" wrote: Get stuffed. Franz |
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#24
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Mitchell Jones wrote:
My own attitude toward this stuff is simple: I seldom argue against generally accepted physics formulae, whether in the area of relativity or elsewhere. The reason is that they have for the most part been verified to good accuracy by the consideration of test cases. Thus my objections to such formulae, if any, tend to lie in the area of *interpretation* rather than in denial that they produce correct answers. For example, when I first pointed out in this group, years ago, that particle accelerators could not test the claim that no material object could exceed lightspeed, because the pushing forces used in accelerators themselves moved at the speed of light... Franz Heymann wrote: The particles have to match the *phase velocity* of the accelerating field It is dead easy to make EM fields propagate with phase velocities greater than c. It is only the group velocity which has an upper limit. ***{It is "dead easy" to make the intersection point of a pair of scissor blades travel faster than light also, if the scissors are long enough and are closed quickly. But, of course, nothing material moves faster than light in that situation, because the intersection point is not a material entity. By the same token, it takes a mere flip of the wrist to make the spot of light projected by a laser pointer travel faster than light, if the surface upon which it is projected is far enough away. But, again, the spot of light is not a material entity. Both the intersection point of the scissors blades and the spot of light are ghosts that have been decreed into existence by an act of stipulation. They represent mere objects of thought, and neither is capable of exerting force on anything that exists. Why not? Because all forces are exerted by particles in collision, and in neither of these cases are there particles which move faster than light. Particles are real entities that have mass and occupy space, and unless you allege that the phase velocity of an electromagnetic wave represents the motion of real entities traveling faster than light, your argument fails. The reason it fails is that ghosts are incapable of exerting force on things which are real. Only real entities can do that. That means an accelerator can test the theory that nothing can travel faster than light only if it strikes the ions which it accelerates with particles that are themselves moving faster than light. Bottom line: to make your argument work, you would have to allege that a phase velocity in excess of lightspeed represents real entities moving faster than light. And, of course, if you do that, you would refute the very point you are trying to prove--to wit: that nothing can travel faster than light. It's real sad! :-) --Mitchell Jones}*** |
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#25
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On 6/18/2004 1:37 AM, Mitchell Jones wrote:
***{It is "dead easy" to make the intersection point of a pair of scissor blades travel faster than light [...] By the same token, it takes a mere flip of the wrist to make the spot of light projected by a laser pointer travel faster than light, Right. Bottom line: to make your argument work, you would have to allege that a phase velocity in excess of lightspeed represents real entities moving faster than light. Not true. Consider a particle traveling westward. If the EM field is generated by structures to the west of the particle and anticipating its arrival, then those structures can arrange IN ADVANCE for the E field to keep up with the particle's motion and accelerate it. In principle this could handle particles traveling faster than c; in practice that never happens. In real particle accelerators this sort of thing occurs -- the RF is ready in advance of the particles' arrival. There is feedback due to longitudinal focusing that ensures that the particles arrive at the proper phase of the accelerating field, as they accelerate; the phases of successive RF cavitries must be set properly to account for the actual travel time of the particles, of course. Accelerators like synchrotrons and linacs could not work without this. [If the accelerator had to work during the initial start-up of the RF, then this could not work. But the RF is a continuous wave, and one can arrange the phases appropriately for particles traveling in the accelerator after the RF is established.] Tom Roberts |
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#26
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"Mitchell Jones" wrote in message ... Mitchell Jones wrote: My own attitude toward this stuff is simple: I seldom argue against generally accepted physics formulae, whether in the area of relativity or elsewhere. The reason is that they have for the most part been verified to good accuracy by the consideration of test cases. Thus my objections to such formulae, if any, tend to lie in the area of *interpretation* rather than in denial that they produce correct answers. For example, when I first pointed out in this group, years ago, that particle accelerators could not test the claim that no material object could exceed lightspeed, because the pushing forces used in accelerators themselves moved at the speed of light... Franz Heymann wrote: The particles have to match the *phase velocity* of the accelerating field It is dead easy to make EM fields propagate with phase velocities greater than c. It is only the group velocity which has an upper limit. ***{It is "dead easy" to make the intersection point of a pair of scissor blades travel faster than light also, if the scissors are long enough and are closed quickly. But, of course, nothing material moves faster than light in that situation, because the intersection point is not a material entity. By the same token, it takes a mere flip of the wrist to make the spot of light projected by a laser pointer travel faster than light, if the surface upon which it is projected is far enough away. But, again, the spot of light is not a material entity. Both the intersection point of the scissors blades and the spot of light are ghosts that have been decreed into existence by an act of stipulation. They represent mere objects of thought, and neither is capable of exerting force on anything that exists. I know. However, you don't appear to appreciate that your analogies fail. The object whose phase I am discussing is an electric field, which is a force per unit charge. it is the phase of this field which is important for accelerating a particle. It iis very easy to make an EM wave with a longitudinal component of E to propagate with a phase velocity les than, equal to or larger than that of light in free space. That longitudinal component is what provides the accelerating force on a charged particle. It has been found possible to make a particle and an RF wave have matched velocities less than c. It has not beem found possible to make the velocity of a particle match that of an RF wave with a phase velocity greater than c. Why not? Because all forces are exerted by particles in collision, and in neither of these cases are there particles which move faster than light. You have now entered drivelling mode. Dragging in quantum mechanical concepts into a purely classical situation shows either a severe lack of understanding or a wilful attempt at throwing sand into the eyes of your readers. Particles are real entities that have mass and occupy space, and unless you allege that the phase velocity of an electromagnetic wave represents the motion of real entities traveling faster than light, your argument fails. An EM field is a real entity. It is dead jammy to obtain circumstances in which an EM field has a phase velocity less than, equal to or larger than c. The only thing that has failed so far is you, failing to understand the argument. The reason it fails is that ghosts are incapable of exerting force on things which are real. Only real entities can do that. That means an accelerator can test the theory that nothing can travel faster than light only if it strikes the ions which it accelerates with particles that are themselves moving faster than light. Balls. Bottom line: to make your argument work, you would have to allege that a phase velocity in excess of lightspeed represents real entities moving faster than light. Yes, the real entity being phase of the the EM field. And, of course, if you do that, you would refute the very point you are trying to prove--to wit: that nothing can travel faster than light. It's real sad! :-) I have maintained that for continued acceleration in an EM wave, a particle must move with the wave in such a way that maintains a position at a constant phase in the wave. That is correct. I have maintained that if the velocity of a piont of constant phase in the wave is less than that of light, it is possible for the particle to maintain a position of constant phase in the wave. That is correct. I have maintained that if the phase velocity of the wave is greater than that of light, the particle is unable to travel at a phase velocity which matches the phase velocity of the wave. That is correct Franz |
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#27
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In article ,
"Franz Heymann" wrote: "Mitchell Jones" wrote: [snip] Bottom line: to make your argument work, you would have to allege that a phase velocity in excess of lightspeed represents real entities moving faster than light. Yes, the real entity being the phase of the the EM field. And, of course, if you do that, you would refute the very point you are trying to prove--to wit: that nothing real can travel faster than light. It's real sad! :-) I have maintained that for continued acceleration in an EM wave, a particle must move with the wave in such a way that it maintains a position at a constant phase in the wave. That is correct. I have maintained that if the velocity of a point of constant phase in the wave is less than that of light, it is possible for the particle to maintain a position of constant phase in the wave. That is correct. I have maintained that if the phase velocity of the wave is greater than that of light, the particle is unable to travel at a phase velocity which matches the phase velocity of the wave. That is correct ***{And you have also maintained (see above) that a real entity--to wit: the phase of the EM field--sometimes moves faster than light. Result: your position is in ruins. Would you like to retract your statement that the phase of the EM field is a real entity which sometimes moves faster than light? --Mitchell Jones}*** Franz |
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#28
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"Franz Heymann" wrote in message ...
"V ertner Vergon" wrote in message om... "Franz Heymann" wrote in message ... "Jim Greenfield" wrote in message m... (V ertner Vergon) wrote in message . com... "Franz Heymann" wrote in message ... Apparently the people running the accellerators "which only work with a phase which produces c" have not realised that a car being towed will NOT exceed c, if the tow-truck is limited to c (no matter how many horses are under the bonnet) Wrong. In an electron linear accelerator, the electron is accelerated by a slow-wave structure in which the phase velocity of the wave is continually matched to the velocity of the electron as it travels along the tube. I take it that you are not aware of the fact that if the final phase velocity exceeds c, the electron falls out of step with the field and ceases to be accelerated. In a synchrocyclotron, the magnetic field is increased steadily as a function of time and sensors determine the RF frequency required to keep the orbits central in the vacuum chamber. If the particle bunches needed a frequency corresponding to a speed greater than c, the feedback system would automatically supply it. Surprise, surprise, the frequency automatically asymptotes to that corresponding to a particle travelling at c. In a microtron, the electrons are left free to choose their own stable orbits. Surprise, surprise, as they get very energetic, they end up by moving on orbits on which they have a velocity c. Franz Vergon: Nothing you say here changes the fact that Jim is correct. A particle can go no faster than the force impelling it. It is the phase of an RF field which determines whether the particle is accelerated or retarded. The phase velocity of an electric field is not limited to c. It is easy to make a linear accelerator in which the phase velocity exceeds c. The trouble is, if you do so, the particle falls out of step. The mass of the particle increases because it absorbs part of the RF impelling it. Simple energy conservation. So what? The collision is part elastic and part inelastic. What collision? What does part elastic and part inelastic mean? An interaction is either elastic or inelastic. Vergon: Wrong. See the analysis of the Compton effect given below. THE COMPTON EFFECT (illustration below) A 1 MeV photon in a direct collision (scattering angle 180 deg) with a free electron (considered at rest) will impart a recoil velocity to it such that E_k = .797 MeV -– [[ Scientific Encyclopedia, Van Nostrand, 5th ed.p. 638 ]]-- Converting the 1 MeV to ergs and utilizing nu = E/h , we ascertain the frequency of the incident photon to be 2.418024 x 10^20. To ascertain the frequency of the recoil photon we utilize [Eq. 2] mc^2 h nu' = ------------------------ mc^2 1 - cos theta + ------ h nu (m = electron mass) ( Continued below after illustration ) %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%% A mass m_q may be assigned to each cycle of frequency which in turn is representative of one individual quantum. m_q = quantum mass = 7.3720385 x 10^-48 gr m_ph = photon mass m_e = electron mass R = Lorentz transformation = sqrt (1 - V^2/c^2) `````````````````````````````````````````````````` `````````````````````` In this work there are a few fundamental physical constants used in a variety of relationships that may not be the same as more modern determinations. Often one that is quite accurate in one relationship does not maintain that accuracy in another but are acceptably close. They a h = 6.625661 x 10^-27 m a d t (erg second) (momenton light second) c = 2.9979254 x 10^10 cm/sec m_e = 9.1089534 x 10^-28 gr (mass of the electron) m_q = 7.37203854 x 10^-48 gr ( mass of the quantum ) `````````````````````````````````````````````````` ````````````````````` MASS AND ENERGY TRANSFER IN A COMPTON COLLISION [Fig. 1] E = h nu = 1.602101 x 10^-6 erg nu = 2.418024 x 10^20 m_ph = 1 MeV = 1.782576 x 10^-27 gr CAPTION FOR Fig. 1 BEFORE AND AFTER COLLISION OF A 1 MeV PHOTON WITH AN "AT REST" ELECTRON. The two spheres at the top are at the moment of contact; those at the bottom are immediately afterward. The incident photon (top left) has almost twice the mass of the electron. The shaded portion is the portion of the incident photon that transfers to the electron on contact. Having mass, this portion carries momentum and energy with it. The quantitative results are exactly the same as those given by relativistic mechanics. _ - - _ ph - |. . . . . . . - e nu = 2.418024 x 10^20 - _ - |. . . . . . . . . . - - - - |. . . . . . . . . . . .- - - - |. . . . . . . . . . . . - - - - |. . . . . . . . . . . . .- - - 3.62763 | . . . . . . . . . . . . .-- - x 10^-28 | 1.419814 x 10^-27 gr . . -- 9.108953 x 10^-28 gr - gr | . . . . . . . . . . . . - - - - | . . . . . . . . . . . . - - - - | . . . . . . . . . . . - - - - | . . . . . . . . . . . - - - - | . . . . . . . . . . - - - | . . . . . . . . . - \ - - - _ _ _ - \ E_k = 0 nu - nu' = 1.925945 x 10^20 \ : \ /\m : \ : _\| e' : - - - _ nu' = 4.920785 x10^19 - . . . . . . |- _ - . . . . . . . . |- - - - . . . . . . . . | - - - - . . . . . . . . . | - - - \ / - . . . . . . . . . . | - - - --* -- - . . . . . . . . . . | - - 3.62763 x 10^-28 - / \ - . . . 2.330709 x 10^-27 gr - - gr - - . . . . . . . . . .| - - - - . . . . . . . . . . | - - _ - - . . . . . . . . . . | - - . . . . . . . . . | - - . . . . . . . . . | - (prime indicates recoil condition) - . . . . . . . . | - - . . . . . . . | - E_ph x .7964954 = E_k_e' - _ . . . .| _ - m_ph x " = /\m - - nu_ph x " = /\nu E_ph x .2035046 = E_ph' m_ph x " = m_ph' nu_ph x " = nu_ph' v = .9204658 c E_k = .7965 MeV (1/R - 1)m_e = /\m = 1.276066 x 10^-6 erg m_e v^2 = /\m c^2 (1/R - 1)m_e c^2 = E_k_e'= -------- R + R^2 m_e' = m_e + /\m = 2.330709 x 10^-27 gr m_e ---- = m_e' nu e' = 3.161554 x 10^20 R %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%% ( Continued from above ) We find the frequency of the scattered photon to be 4.920785 x 10^19, a frequency loss nu - nu' of 1.925946 x 10^20. Since each element of the frequency represents a quantum, this figure represents the quantity of quanta n lost to the photon and absorbed by the electron. Thus (nm_q) = /\ m_ph = /\ m_e = 1.419814 x10^-27 gr and is the mass transferred. The energy of this mass is (nm_q^c2) = 1.276066 x 10^-6 erg (h nu) which manifests as kinetic energy transferred to the recoil electron. This converts to .7965 MeV which agrees quite well with the .797 MeV of experiment. The only energy imparted to the electron is that contained in /\ m_ph. Thereby /\ m_ph c^2 is converted to (1/R - 1) m_e c^2 [Eq. 3] Thus /\ m_ph c^2 = (1/R - 1) m_e c^2 [Eq. 4] Therefore /\ m_ph = (1/R -1) m_e [Eq. 5] Finally /\ m_ph = (m_e/R - m_e) = /\ m_e [Eq. 6] which clearly demonstrates that the relativistic expression in the center is nothing other than the mass, /\m_ph, absorbed from the photon and which carries the total kinetic energy now resident in the recoil electron (on the assumption that the free electron is considered essentially at rest. For clarification, we can write Eq. 6 as [Eq. 6A] m_e --- = (m_e + /\ m_ph) = (m_e + /\m_e) R Hence the term "increase in inertial mass" has a clear mechanistic explanation not forthcoming in relativity theory. Note, this is so only for e.m. accelerated particles. We also note from Eq. 6A that the ratio of the electron mass before and after absorption is equal to the Lorentz transformation: m_e ---------------- = R . m_e + /\ m_e and Eq. 5 shows that (1/R -1) m_e is the quantity of mass transferred in the collision. We summarize the conditions: If the quanta absorbed by the electron is nu - nu' = nu'' = n , then E_k = h nu'' = (nm_q) c^2 = /\ m_ph c^2 = (1/R - 1) m_e c^2 . from which we can readily calculate R and v. The shaded portion of the incident photon is the /\ m_ph that transfers in the collision, imparting a velocity of 92% c. The rebounding photon, having suffered the loss of /\ m has a frequency that is lowered by /\ m/m_q. The percentage loss of mass by the photon is /\ m_ph/m_ph x 100. This is a 79.65 % inelastic collision. Consequently, that is the Percentage of the photon mass transferred m_ph x .7964952 = 1.419814 x 10^-27 gr = /\m Do you actually have any inkling of what you are posting about? And in case you are not aware, you lost the argument re the addition of velocities. Nope. Franz |
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#29
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"Mitchell Jones" wrote in message ... In article , "Franz Heymann" wrote: "Mitchell Jones" wrote: [snip] Bottom line: to make your argument work, you would have to allege that a phase velocity in excess of lightspeed represents real entities moving faster than light. Yes, the real entity being the phase of the the EM field. And, of course, if you do that, you would refute the very point you are trying to prove--to wit: that nothing real can travel faster than light. It's real sad! :-) I have maintained that for continued acceleration in an EM wave, a particle must move with the wave in such a way that it maintains a position at a constant phase in the wave. That is correct. I have maintained that if the velocity of a point of constant phase in the wave is less than that of light, it is possible for the particle to maintain a position of constant phase in the wave. That is correct. I have maintained that if the phase velocity of the wave is greater than that of light, the particle is unable to travel at a phase velocity which matches the phase velocity of the wave. That is correct ***{And you have also maintained (see above) that a real entity--to wit: the phase of the EM field--sometimes moves faster than light. Result: your position is in ruins. Just as an example, the phase velocity of any EM wave in a normal rectangular waveguide with plane surfaces is always larger than c. You have made it clear that you have no notion of the propagation of EM radiation. Would you like to retract your statement that the phase of the EM field is a real entity which sometimes moves faster than light? Of course not. What you need to bone up on is precisely what SR says can not move faster than light. The indications so far are that you have not a clue about the situation. Franz |
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#30
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"V ertner Vergon" wrote in message om... "Franz Heymann" wrote in message ... "V ertner Vergon" wrote in message om... "Franz Heymann" wrote in message ... "Jim Greenfield" wrote in message m... (V ertner Vergon) wrote in message . com... "Franz Heymann" wrote in message ... Apparently the people running the accellerators "which only work with a phase which produces c" have not realised that a car being towed will NOT exceed c, if the tow-truck is limited to c (no matter how many horses are under the bonnet) Wrong. In an electron linear accelerator, the electron is accelerated by a slow-wave structure in which the phase velocity of the wave is continually matched to the velocity of the electron as it travels along the tube. I take it that you are not aware of the fact that if the final phase velocity exceeds c, the electron falls out of step with the field and ceases to be accelerated. In a synchrocyclotron, the magnetic field is increased steadily as a function of time and sensors determine the RF frequency required to keep the orbits central in the vacuum chamber. If the particle bunches needed a frequency corresponding to a speed greater than c, the feedback system would automatically supply it. Surprise, surprise, the frequency automatically asymptotes to that corresponding to a particle travelling at c. In a microtron, the electrons are left free to choose their own stable orbits. Surprise, surprise, as they get very energetic, they end up by moving on orbits on which they have a velocity c. Franz Vergon: Nothing you say here changes the fact that Jim is correct. A particle can go no faster than the force impelling it. It is the phase of an RF field which determines whether the particle is accelerated or retarded. The phase velocity of an electric field is not limited to c. It is easy to make a linear accelerator in which the phase velocity exceeds c. The trouble is, if you do so, the particle falls out of step. The mass of the particle increases because it absorbs part of the RF impelling it. Simple energy conservation. So what? The collision is part elastic and part inelastic. What collision? What does part elastic and part inelastic mean? An interaction is either elastic or inelastic. Vergon: Wrong. No, I was right. You need to learn something about kinematics and about interactions before deeming yourself educated enough to spout on the subject. In the meantime, you are simply emitting horse dung. See the analysis of the Compton effect given below. THE COMPTON EFFECT [snip] You simply cribbed that calculation which I snipped from somewhere without knowing what you cribbed, otherwise you would have realised that the interaction you were talking about was a perfectly elastic interaction. Do you know what the definition of an elastic interaction is? Do you know what the definition of an inelastic interaction is? Do you actually have any inkling of what you are posting about? And in case you are not aware, you lost the argument re the addition of velocities. Nope. Franz |
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