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Because of the other electrons imparting a restoring force? Assuming that would work (which it doesn't, as has been shown numerous times) you then have the problem of energy being diffused through the system... Quote:
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Cheers, Lyndon |
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Cheers, Lyndon |
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Cheers, Lyndon |
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Just kidding, but the whole theory is becoming so nonsensical that kidding is all that is left to do...
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Knowledge is a curse, but ignorance is worse |
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I am quoting this post:
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It is Lyndon's error... not anyone else's.... to fail to account for the inevitable transverse impulse and consequent scatter that always arises in photon-electron interactions. In real physics, there is always a transverse component, and therefore always a scatter angle for the photon. Many BABB contributors are inclined to think these discussions are a waste of time. I don't agree. The point is not to teach Lyndon anything... that is plainly impossible. But looking into each new error and distraction is a chance to learn something, even if Lyndon himself never avails himself of the opportunity. So how does photo-absorption occur in real physics? Don't physicists speak of electrons absorbing photons? Can't the objections I am raising carry over to photo-absorption or electron-photon interactions proposed in text books?
This serves to demonstrate that in real physics, you should get the same answer, even if you apply different kinds of analysis to the problem. No matter which way you look at it, Lyndon's interaction is impossible.
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This oscillation only occurs while the electron is still interacting with the photon's electromagnetic fields. Once the photon is gone (either absorbed or emitted) this oscillation is over, and all that is left is a small residual impulse on the electron. Lyndon proposes that a photon is absorbed. So where does the energy go? He can't appeal to the oscillations that occur while the photon is still involved. It's gone mate, by his own description. Quote:
If you want to involve other particles a meter or more away, be my guest, but quantify the forces involved. If the energy ends up in motions of any other particles, then you also have to get it all back to power the emission of a redshifted photon! Here is Lyndon's attempt to manage the energy momentum budget. I have highlighted in blue one particularly reprehensible bit of deliberate dishonesty; and I shall show some trivial errors that make this unacceptable even for high school level. Quote:
This is dishonest. The above still fails to be an energy-momentum budget, because it never mentions the momentum! Momentum of electron = sqrt(2Em) = 8.51e-25 kg m/s. Initial momentum of the 500 nm photon = 1.33e-27 kg m/s. Now the momentum does not balance. The magnitudes differ by a factor of 642! In his own paper, Lyndon calculates kinetic energy for the electron as 9.65e-25, using conservation of momentum. [[See formula Q^2/2mc^2 on the bottom of page 3, and plug in the numbers.]] That is the energy for the electron that belongs in the above picture. A high school physics student should be able to figure out how to give a quantified energy momentum budget. You have to calculate numbers for energy, and numbers for momentum, and show that they balance. Lyndon has never done this. Cheers -- Sylas PS. I had not heard of the Mössbauer Effect before reading Lyndon's stuff. Initially I accepted his description of straight line transmission with no scatter, and repeated it myself in some posts. I now suspect this is wrong, and that photons can be scatted in all directions. The distinguishing feature is not a lack of scatter, but negligible recoil in the atom, and hence negligible change in wavelength. I'll be checking this further to confirm or retract; whether I'm right or wrong I'll have learned something. [[Edit to fix a typo in one formula; numbers unchanged.]] |
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This is the typical situation for Mössbauer effect. Take a crystal lattice containing radioactive (gamma emitting) Iron isotopes. The excited Iron nuclei emit gamma photons. If the energy of that photon is lower than the energy necessary to excite a phonon (quantum of lattice vibrations), the emission of the gamma photon is effectively recoil-less. The recoil is transferred to the whole crystal (10^23 atoms), rather than to the emitting atom (which would make the atom vibrate in the lattice). The spectral line corresponding to this recoil-less emission, is very narrow, and makes some nice experiments possible. For example, it has been used to measure gravitational red-shift on Earth, between the basement and the top of a tower. In a teaching lab, I used it to measure the hyperfine field in Iron.
__________________
papageno "Why waste time learning, when ignorance is instantaneous?" - Hobbes (Calvin and Hobbes) "It's all about context!" - Vince Noir (The Mighty Boosh) "I've never heard of such a brutal and shocking injustice that I cared so little about!" - Zapp Brannigan (Futurama) "...because the logic of the lines traced from reality is as poor of aesthetic value as it is strict in consistency. " - Paolo Bozzi (Naive Physics - free translation) |
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As a test of my understanding... it seems to me that the recoil-less emission should mean that photons can be absorbed by an atom, and then re-emitted with exactly the same frequency to all intents and purposes, with no energy loss to the lattice. The re-emitted photon can continue to pass through the lattice, possibly being absorbed and re-emitted a number of times, all with no loss of energy. But so far I see nothing to constrain it to remain in a straight line. I've seen references compare this with "resonance fluorescence of the yellow D lines of sodium in sodium vapour". See, for example Recoilless nuclear resonance absorption of gamma radiation, which is Rudolf Mössbauer's Nobel lecture. In this case, the fluorescence means that the whole gas glows as photons bounce around within the gas. I guess the same thing happens for gamma photons in a crystal lattice at the excitation frequency of the Mössbauer effect. If a beam of gamma ray photons of exactly the right frequency are directed into the lattice, I would expect to see photons emerging from the lattice at the same frequency and in every possible direction. Have I got this right? When I first read Lyndon's paper, I got the impression that Mössbauer effect meant that the photons had no scatter angle, but now I think this is just another error on Lyndon's part. Or perhaps it is my error and I have misunderstood Mössbauer's lecture. Unless I am badly mistaken, Lyndon's effect is completely the opposite of the Mössbauer effect in all the essential respects:
It is the last point on which I am least certain. Thanks for any help -- Sylas |
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However, the Earth's mass is so much larger than yours, that the recoil is negligibly small. Quote:
Whether the emission (absorption does not seem very likely, since the gamma photon needs to hit a nucleus) is recoil-less, depends on the lattice. The phonon spectrum is not necessarily isotropic, so you might have absence of recoil in one direction, but recoil in another direction even though the energy is the same. The emission by the nucleus is isotropic.* Quote:
However, I do not expect absence of recoil in gas atoms, because the atom are not constrained. So I would expect broadening of the spectral line in the fluorescent emission. Quote:
Then you have to consider the spectrum of the lattice vibrations, to see when recoil is absent. Quote:
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Normal emission: jumping from a spring-board. Mössbauer emission: jumping from a hard concrete wall. * Well, it depends on magnetic field and temperature. For anisotropic gamma emission, search for low temperature nuclear orientation.
__________________
papageno "Why waste time learning, when ignorance is instantaneous?" - Hobbes (Calvin and Hobbes) "It's all about context!" - Vince Noir (The Mighty Boosh) "I've never heard of such a brutal and shocking injustice that I cared so little about!" - Zapp Brannigan (Futurama) "...because the logic of the lines traced from reality is as poor of aesthetic value as it is strict in consistency. " - Paolo Bozzi (Naive Physics - free translation) |
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Hi Sylas,
I am still awaiting a reply to my post. The long 'epistle according to Sylas' above answers nothing but repeats all your wrong sums. You have spent the last 20 odd pages treating light as a longitudinal wave. This has been pointed out to you time and time again. We would like a response. In using mv^2/2 to represent the whole of the photon energy, using v as the recoil velocity, you are saying light is longitudinal. Can we have a response to this point please, and then you can go on to proving Mr Mossbauer wrong. Cheers, Lyndon |
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I will repeat the last issue I had... Quote:
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It isn't vague at all. momentum is only conserved if there are no external forces acting. In "physics according to Sylas volume 1" he expects momentum to be conserved, but we don't. The momentum of the electron in a direction perpendicular to that in which the photon was originally travelling is not conserved because there is an external force acting on it - due to the oscillating electric fields of the photon. This is why it gains energy and momentum in this direction. If one wants momentum to be conserved then one must look at the universe as a whole - including when the photon was transmitted. A wibbly wobbly when it was created is cancelled by a wibbly wobbly when it was absorbed. Cheers, Lyndon If one momentum |
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The frequency of oscillation of the electrons about 1m apart in plasma of IG space is a published result, about 30 or less hertz. In any case, this is how light travels through glass. I am not inventing anything new here on this point, I am just applying known physics of transparent materials to space. And getting the correct answers - H = 2nhr/m. Cheers, Lyndon. |
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My analysis has been simply conservation of momentum. Invoking the wave directions does not absolve you from the responsibility of balancing the initial momentum with the momentum of the final state. You have a photon with momentum in a certain direction. That momentum must be conserved, and it is not conserved in your reaction. You can do an energy momentum budget just by adding up the energy and momentum of all the particles involved in the reaction. I take it back. High school students can do energy momentum budgets; but we have yet to see a complete balanced budget from Lyndon, that takes both energy and momentum into account and shows them conserved. But let's talk about waves, if you prefer that approach. This gives another proof that the photo-absorption by an electron is impossible. The wave is longitudinal. It therefore gives the electron a push to one side. Therefore the photon cannot be absorbed, since it must go off to the opposite side to counterbalance. Equal and opposite reactions -- but violated if the photon is absorbed. Therefore absorption is impossible. If you EVER get around to doing a complete energy momentum budget, you will have to consider that the electron DOES get pushed sideways, and you have to find SOMETHING ELSE pushed the other way to balance. In real physics of photoabsorption, it is the positive nucleus. In real physics of Compton effect, it is a scattered photon. In the Lyndon effect, there is nothing to compensate the sideways movement of the electron, and so the effect is a violation of trivial school level physics. Cheers -- Sylas |
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You are always going on about what you see as his wrong sums and random numbers, but you don't give anything better or even a good reason why we should doubt Sylas.
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Knowledge is a curse, but ignorance is worse |
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Similarly, if we have a photon interacting with a plasma, we can consider just the plasma and the photon as a closed system. If there are other outside forces involved with the photon and the plasma that prevent conservation of momentum and energy, you should be able to identify and calculate them. If not, you should be able to work out the details, assuming that only the photon and the plasma are involved, yet you've failed, again, to give a quantitative analysis of the matter. If only including three electrons (the one doing the absorption and its nearest neighbors, presumably) won't allow you to do a quantitative analysis, then first I'll ask why you brought up that model in response to questions about conservation of energy and momentum. And second, I'd expect you to expand your simple model, so that you can show it. Remember, burden of proof here is on you, if you expect to convince anyone to take your ideas seriously. Quote:
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I'm sure you meant to say that the wave is transverse here (especially since you then speak about the wave being deflected to the side, which wouldn't be the case for a longitudinal wave, so it looks like a mistake of words rather than one of logic). Perhaps having Lyndon continually saying that you're treating the wave as longitudinal left you with that word on your brain. ![]() |
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I didn't ask for the oscillation frequency, I asked for the amount of time between photon-absorbtion and photon emission. I'm not the first to ask this. So how long is it? You also failed to answer the question of how a system of electrons produces a single photon. How does a system of electrons suddenly behave as one to produce a photon? Where is the photon emitted from, exactly? By what process is it emitted? How does the system know where to fire it to prevent scatter? Edited to clarify questions |
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He has worked out the recoil velocity of the electron and, when he finds that he cannot equate the energy of the photon with that picked up in recoil, he says "where has the energy gone" . In transwerse waves they are separate entities. One deducts the energy picked up in recoil from the energy of the photon and it is this that produces the redshift. Cheers, Lyndon |
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__________________
Some try to tell me, thoughts they cannot defend,... - Moody Blues. Neptune- The original Dark Matter. The author feels that this technique of deliberately lying will actually make it easier for you to learn the ideas. - Donald Knuth |
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I have shown my working many times over. Conservation of energy and momentum is BUILT IN TO MY CALCULATIONS I work out how much momentum and hence energy the electron gains assuming conservation of momentum. I assume conservation of energy and deduct the energy gained by the recoiling electron from that of the incident photon to get the redshift. They have to apply because I have built them in to my calaculations. Additionally, Sylas has shown us his sums and I have shown him time and time over where his sums are wrong. The matter is settled, lets move on. Light is transverse - trust me. Cheers, Lyndon |
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Those "oscillating electric fields of the photon" would not be an external force: their would be the internal force responsible for the electron-photon scattering. The only external force in the scattering of the electron and the photon is the Coulomb interaction with the other charged particles in the plasma. You have mto show that the time interval in which the electron-photon scattering occurs, is long enough for the external forces to have any effect on the system. I urge you again to take the BA's warning seriously, and address the point: provide your full calculations in support of the basic mechanism for your "theory". Stop hand-waving and tap-dancing around the issue. Your broken-record tactic does not equal addressing the point.
__________________
papageno "Why waste time learning, when ignorance is instantaneous?" - Hobbes (Calvin and Hobbes) "It's all about context!" - Vince Noir (The Mighty Boosh) "I've never heard of such a brutal and shocking injustice that I cared so little about!" - Zapp Brannigan (Futurama) "...because the logic of the lines traced from reality is as poor of aesthetic value as it is strict in consistency. " - Paolo Bozzi (Naive Physics - free translation) |
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But lets look at things in more detail. I seem to be cast as the 'bad guy' in all this (which is totally untrue 'cos I am quite nice) so lets have a look at some of Sylas' sums that you all seem to agree with. On page 20 Sylas said: Quote:
On page 22 we have, Quote:
But wait a minute, 400,000 electrons to absorb a single photon of light? Hydrogen atoms can not only absorb certain wavelengths of light of this order but they can absorb photons with much more momentum and energy in the UV - and do it individually as atoms in a gas. Hydrogen atom has a mass of about 2000 electrons so why does Sylas need the equivalent of 400,000 electrons to absorb a single photon of light. Rubbish. He is saying that unless you have 200 Hydrogen atoms the momentum/ energy ‘budget’ doesn’t work when a hydrogen atom is excited by a single photon. I have explained were he is going wrong but the guy won't listen. I have no intention of trying to repeat this sort of nonsense. Quote:
Cheers, Lyndon |
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