Tor Fredrik Posted December 21, 2019 Posted December 21, 2019 (edited) the theory above from physics stack exchane made me puzzle a little One set of possible solutions to maxwell equations are It is known that deacceleration of an electron creates EM-waves. If you have a constant acceleration of an electron from a B field and stops the electron then all kinetic energy should be given out as an EM-wave so that Anyone have anything to add of an experiment that could determine the frequency this way? Edited December 21, 2019 by Tor Fredrik
swansont Posted December 21, 2019 Posted December 21, 2019 1 hour ago, Tor Fredrik said: the theory above from physics stack exchane made me puzzle a little One set of possible solutions to maxwell equations are It is known that deacceleration of an electron creates EM-waves. If you have a constant acceleration of an electron from a B field and stops the electron then all kinetic energy should be given out as an EM-wave so that Anyone have anything to add of an experiment that could determine the frequency this way? A B field won’t stop an electron, and would not represent a constant acceleration. Also, a photon in a cavity is a different problem from Bremsstrahlung.
Tor Fredrik Posted December 21, 2019 Author Posted December 21, 2019 (edited) 2 minutes ago, swansont said: A B field won’t stop an electron, and would not represent a constant acceleration. well what if we just stopped an electron with kinetic energy and then equated this as the energy of the EM-wave released? Edited December 21, 2019 by Tor Fredrik
swansont Posted December 21, 2019 Posted December 21, 2019 3 minutes ago, Tor Fredrik said: well what if we just stopped an electron with kinetic energy and then equated this as the energy of the EM-wave released? If you converted all the energy, then KE = hbar*omega. It would represent the maximum frequency in case there were losses. But you have to have a situation where you only get one photon.
Tor Fredrik Posted December 21, 2019 Author Posted December 21, 2019 Just now, swansont said: If you converted all the energy, then KE = hbar*omega. It would represent the maximum frequency in case there were losses. But you have to have a situation where you only get one photon. well I thought E=hf is only valid for photons?
swansont Posted December 21, 2019 Posted December 21, 2019 4 minutes ago, Tor Fredrik said: well I thought E=hf is only valid for photons? What’s the problem? A 1 keV electron being stopped can give you a photon of maximum 1 keV. Its frequency would be given by hf
Tor Fredrik Posted December 21, 2019 Author Posted December 21, 2019 (edited) 3 minutes ago, swansont said: Yes. What’s the problem? A 1 keV electron being stopped can give you a photon of maximum 1 keV. Its frequency would be given by hf Well with my calculations there would be a formula for finding frequency f without using E=hf? But I needed clarifications since the solutions to maxwell dont directly tell me how to quantify its energy. Edited December 21, 2019 by Tor Fredrik
swansont Posted December 21, 2019 Posted December 21, 2019 31 minutes ago, Tor Fredrik said: Well with my calculations there would be a formula for finding frequency f without using E=hf? But I needed clarifications since the solutions to maxwell dont directly tell me how to quantify its energy. Maxwell doesn’t tell you how many photons you have. But there have to be an integral number, so you can check to see it’s at least consistent.
Tor Fredrik Posted December 21, 2019 Author Posted December 21, 2019 Just now, swansont said: Maxwell doesn’t tell you how many photons you have. But there have to be an integral number, so you can check to see it’s at least consistent. Is there a way to calculate this?
swansont Posted December 21, 2019 Posted December 21, 2019 Just now, Tor Fredrik said: Is there a way to calculate this? The ratio of the frequency from E=hf and your calculation should be an integer. 1
Enthalpy Posted December 21, 2019 Posted December 21, 2019 Hi Tor Fredrik, Swansont and everyone, I'm not sure of the classical energy formula you propose for the EM wave in the box. Electric and magnetic energy, but they are not present at the same time in a standing wave. If said box is a resonator, the constant contained energy oscillates between electric and magnetic form. Also, if the distribution is like sin(x)*sin(y)*sin(z), each dimension loses a factor of 2 in the mean versus peak energy density. What kind of frequency do you want to measure? When I'm an electrical engineer, I can measure the resonant frequency of a cavity. Shall the photons' frequency differ from the cavity's resonance? Big cavity and small wavelength? I don't see figures in your proposal. Technological electrons in vacuum tend to have >100eV energy (up to very much) and are produced by cathodes 0.05eV-0.2eV hot, which makes low energies inaccurate. But 100eV is already UV or X-rays, with 12nm wavelength. How small shall the box be? EM standing waves are used to produce energetic photons by interacting with energetic electrons. Call it Bremsstrahlung if you wish, it's the same and it works. But did you check how hugely inefficient Bremsstrahlung is? In storage rings they have >1T but one or few photons produce an extremely faint induction. In the setups to make energetic photons, they concentrate very powerful laser light in a resonator with dichroic mirrors to have a huge light power density. Very far from few photons. I may be way off, but I imagine Haroche-style experiments with GHz photons in a superconducting cavity. I know no other lossless box. 3GHz is only 12.4µeV. 1
Tor Fredrik Posted December 27, 2019 Author Posted December 27, 2019 (edited) In the theory aove they calculate the perturbation of an E-field. Since there is kinetic energy involved I thought perhaps that the energy also could be emitted as an EM-wave. The issue is that they dont adress the mass of the moving part of the infinte sheet. If that mass was known one could use kinetic energy as well. Then I have for equalities: Is it possible to isolate them for h without having f or B as a variable? Edited December 27, 2019 by Tor Fredrik
swansont Posted December 27, 2019 Posted December 27, 2019 12 minutes ago, Tor Fredrik said: In the theory aove they calculate the perturbation of an E-field. Since there is kinetic energy involved I thought perhaps that the energy also could be emitted as an EM-wave. It flat-out tells you it's carried off as an EM wave.
Tor Fredrik Posted January 5, 2020 Author Posted January 5, 2020 When the coil has turned 90 degrees it reaches equilibrium and deaccelerates to 0 velocity. Lets assume hypotetically that all this energy is released as one photon. Now I will try to introduce radiation pressure: So we hypotetically want the electron that has been deaccelerated to 0 velocity (I will ignore the current direction) to obtain the same kinetic energy and velocity. We want it to absorb a photon to do so. If we look at one half cycle of an EM wave that would be half of the energy of one photon if all of the energy of the photon is contained in one cycle. The EM wave exert radiation pressure as described above. It is also said that E=pc where p is radiation pressure density and E is energy density. Over a half cycle of an EM wave the avearge cycle can be obtained the following way: In order to calculate the amplitude of the EM wave I try the following: First I calculate the kinetic energy from the 90 degrees turn of the circular coil Then I try to find the amplitude of the EM wave and uses the theory for the radiation pressure above along with E=pc: Is this a wrong usage of the radiation pressure?
swansont Posted January 5, 2020 Posted January 5, 2020 12 hours ago, Tor Fredrik said: When the coil has turned 90 degrees it reaches equilibrium and deaccelerates to 0 velocity. Why would it do that? The torque drops to zero, but there would still be a angular speed Quote So we hypotetically want the electron that has been deaccelerated to 0 velocity (I will ignore the current direction) to obtain the same kinetic energy and velocity. We want it to absorb a photon to do so. A photon cannot be absorbed by a free electron. Quote If we look at one half cycle of an EM wave that would be half of the energy of one photon if all of the energy of the photon is contained in one cycle. The EM wave exert radiation pressure as described above. It is also said that E=pc where p is radiation pressure density and E is energy density. E is energy and p is momentum 1
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