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Eric Gisse says...
On Mar 26, 2:42=A0pm, Koobee Wublee wrote: What is the transverse Doppler effect under relativity? =A0According to the energy transformation and also your derivation, it should predict a blue shift while experiments time after time all have indicated red. oops! oshrug In what way are your arguments credible? It has already been established that you were COMPLETELY WRONG when discussing your strawman derivation of the relativistic Doppler effect. What are the odds you are correct about the transverse Doppler effect? Koobee's problem is that physics is hard, and Koobee is lazy. Whenever he runs into something that he doesn't understand, he gives up, and declares it to be nonsense. But Koobee has noticed an ambiguity in the interpretation of the phrase "the transverse Doppler effect". That's actually to his credit. But rather than trying to *resolve* the ambiguity, he's taking at as yet another argument that relativity is nonsense. I could explain the situation to him, but Koobee is incapable of following arguments that require thought, and dismisses them as "fudging". The question is: What is the formula for the transverse relativistic Doppler effect? Let's add some background information to make this question more precise: Suppose we have two observers, A and B, traveling inertially. Let F be the frame in which A is at rest, and let F' be the frame in which B is at rest. Assume that, according to the coordinate system of frame F, B is traveling in the +x direction at speed v. Rather than assuming that the separation between A and B is in the x-direction, we will assume that they are at different y locations. For definiteness, we will assume that, as measured in frame F, B is traveling in the x-direction along the line y=L, and A is sitting at x=0, y=0. Assume that A is transmitting a periodic electromagnetic wave in the +y direction. Let e_1 be the event at A corresponding to the start of a cycle, and let e_2 be the event at A corresponding to the end of that cycle. Let T be the time between e_1 and e_2, in frame F, which is also the period of the wave. Now, about this set up, we can ask two *different* questions about what things look like in frame F': (1) Let T'' be the period of the electromagnetic wave produced by A, as measured by frame F'. What is the ratio T''/T? (2) Let e_3 be the event at which the signal from event e_1 reaches the line y=L. Let e_4 be the event at which the signal from event e_2 reaches the line y=L. Let T' be the time between e_3 and e_4, as measured in frame F'. What is the ratio T'/T? If B were traveling in the same direction as the electromagnetic wave, straight away from A, then there would be no difference between T' and T''. But in the transverse case, they are not the same. This is not an inconsistency; the two quantities T' and T'' have different definitions, and there is no logical reason for them to be equal, and they are not equal according to SR. Solution to (1). The simplest to derive is T''. The phase phi of the electromagnetic wave is given in frame F by phi = k y - w t, where k = w/c and where w = 2pi/T. Phase is an invariant. So when we switch to frame F', we have: phi' = phi = k y - w t We want to re-express this in terms of F' coordinates, so we use the inverse Lorentz transform: y = y' t = gamma (t' + v/c^2 x') to get phi' = k y' - gamma w t' - gamma vw/c^2 x' We can write this in the form: phi' = k_x' x' + k_y' y' - w' t' with the definitions: k_x' = - gamma vw/c^2 k_y' = k w' = gamma w Since w' = 2pi/period, we defined T'' to be the period in F', we have: T'' = 2pi/w' = 2pi/(gamma w) = 1/gamma (2pi/w) = T/gamma So T''/T = 1/gamma. So T'' is less than T, by a factor of 1/gamma. Solution to (2). To derive T', we need to compute the coordinates of the events e_1, e_2, e_3 and e_4 in both frames. Once again, e_1 is the event at sender A at rest in the F frame at the start of a cycle. e_2 is the event at sender A at the end of the same cycle (time T later, according to frame F). e_3 is the event at which the light from e_1 crosses the line y=L. e_4 is the event at which the light from e_2 crosses y=L. e_1 and e_2 take place at A, which we can assume is the origin of the F coordinate system. We may as well assume that e_1 takes place at t=0. So we have: x_1 = 0 y_1 = 0 t_1 = 0 x_2 = 0 y_2 = 0 t_2 = T Light propagating in the y-direction will reach the line y=L after a time period of L/c. So we have: x_3 = 0 y_3 = L t_3 = L/c x_4 = 0 y_4 = L t_4 = T + L/c Letting delta-x be x_4 - x_3, delta-y be y_4 - y_3, and delta-t be t_4 - t_3, we have: delta-x = 0 delta-y = 0 delta-t = T Now, transform to frame F' to get: delta-x' = - gamma vT delta-y' = 0 delta-t' = gamma T delta-t' is just the T' introduced earlier. So we have: T'/T = gamma So T' is greater than T, by a factor of gamma. Reconciliation of (1) and (2). As we saw, T' and T'' are not the same: T' T, but T'' T. But the two results are completely compatible. Let's look at the change in phase between e_3 and e_4 in both frames. In frame F, the phase is given by: phi = ky - wt, so the change in phase between e_3 and e_4 is delta-phi = k delta-y - w delta-t = 0 - wT = - 2pi (because w = 2pi/T) Now, look at the same change in phase from the point of view of frame F': delta-phi = k_x' delta-x' + k_y' delta-y' - w' delta-t' We've already calculated k_x' = - gamma vw/c^2 k_y' = k w' = gamma w delta-x' = - gamma vT delta-t' = gamma T So delta-phi = (- gamma vw/c^2)(- gamma vT) + 0 - (gamma w) (gamma T) = gamma^2 v^2/c^2 wT - gamma^2 wT = -gamma^2 wT (1-v^2/c^2) = - wT (since gamma^2 = 1/(1-v^2/c^2)) = -2pi So the two equations T' = gamma T and T'' = 1/gamma T are perfectly consistent, once you realize that T' is *NOT* the period of the electromagnetic wave in frame F'. Why not? It's because e_3 and e_4 are not at the same location in frame F'; they don't have the same value for x'. To directly compute the period of a wave, you have to have two events such that the first event is at the start of one cycle (which is the case with e_3), and the second event is at the end of that cycle (which is the case with e_4), and the two events are at the *SAME* location (which is not the case with e_3 and e_4). So the time between e_3 and e_4 is NOT the period in frame F'. -- Daryl McCullough Ithaca, NY |
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On Mar 27, 9:01 am, Daryl McCullough wrote:
On Mar 26, Koobee Wublee wrote: What is the transverse Doppler effect under relativity? According to the energy transformation and also your derivation, it should predict a blue shift while experiments time after time all have indicated red. Oops! shrug This disagreement of SR with experiments is serious and fatal, no? [So] checkmate Koobee's problem... It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** [v] = Velocity vector between frames of f and f ** [c] = Velocity vector of light ** [] * [] = dot product of two vectors Under the transverse case, ** f / f = 1 / sqrt(1 v^2 / c^2) Where ** [v] * [c] = 0 This means SR predicts a blue Doppler shift in the transverse direction, and that is totally wrong. shrug Anyone with half a brain would attempt to execute a graceful retreat from that. shrug It smells like a bunch of sour ass losers with unsportsmanlike conducts. shrug The bottom line is that SR does not produce what is observed in experiments. Thus, SR is merely garbage. Just how difficult can that be? shrug |
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On Mar 27, 9:28*pm, Koobee Wublee wrote:
On Mar 27, 9:01 am, Daryl McCullough wrote: On Mar 26, Koobee Wublee wrote: What is the transverse Doppler effect under relativity? According to the energy transformation and also your derivation, it should predict a blue shift while experiments time after time all have indicated red. *Oops! *shrug This disagreement of SR with experiments is serious and fatal, no? [So] checkmate Koobee's problem... It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** *f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Its' already been established that you don't know how to derive anything in relativity. What's the point in going over old ground? [snip rest, unread] |
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Koobee Wublee says...
On Mar 27, 9:01 am, Daryl McCullough wrote: On Mar 26, Koobee Wublee wrote: What is the transverse Doppler effect under relativity? According to the energy transformation and also your derivation, it should predict a blue shift while experiments time after time all have indicated red. Oops! shrug This disagreement of SR with experiments is serious and fatal, no? [So] checkmate You are deeply confused. You haven't pointed out any disagreements. It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. You never derive any of your results, which makes them useless for the purposes of discussion. You have made claims, without deriving those claims, and every single claim has proved to be false. As I explained, there are two different questions: (1) Given an electromagnetic wave described by attributes: k_x, k_y, k_z, w in one frame F, what are the attributes in the frame F' of an observer moving at speed v in the x-direction relative to F? This is easily answered by realizing that phase is an invariant. So k_x x + k_y y + k_z z - w t = k_x gamma (x' + v t') + k_y y' + k_z z' - w gamma (t' + v/c^2 x') = gamma (k_x - wv/c^2) x' + k_y y' + k_z z' - gamma (w - k_x v) t' So it is clear that in frame F', the wave attributes are given by: k_x' = gamma (k_x - wv/c^2) k_y' = k_y k_z' = k_z w' = gamma (w - k_x v) This is exactly the same as the transformation of the energy-momentum four-vector: p_x' = gamma (p_x - Ev/c^2) p_y' = p_y p_z' = p_z E' = gamma (E - p_x v) I don't know why you think that there is some kind of incompatibility. This means SR predicts a blue Doppler shift in the transverse direction, and that is totally wrong According to what, or who? The bottom line is that SR does not produce what is observed in experiments. The bottom line is that you have made many false claims and that's another. -- Daryl McCullough Ithaca, NY |
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Koobee Wublee says...
On Mar 27, 9:01 am, Daryl McCullough wrote: On Mar 26, Koobee Wublee wrote: What is the transverse Doppler effect under relativity? According to the energy transformation and also your derivation, it should predict a blue shift while experiments time after time all have indicated red. Oops! shrug This disagreement of SR with experiments is serious and fatal, no? [So] checkmate Koobee's problem... It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** f'/f = (1 + [v] * [c]) / sqrt(1 - v^2 / c^2) Under the transverse case, ** f' / f = 1 / sqrt(1 - v^2 / c^2) It's kind of funny that you should quote these as evidence that I'm wrong, when I derived exactly those results. But the transverse result you give is *NOT* describing how the frequency of an electromagnetic wave changes under a change of coordinate systems. Instead, it is a description of the ratio of frequencies of sending and receiving signals. Why are these not the same thing? Well, I explained why not, in another post. The scenario is this: We have two inertial observers, A and B. According to A's frame, A is at rest at location x=0, y=0. B is traveling in the +x direction along the line y=L. A is transmitting signals in the +y direction. Now, think about it: B is moving perpendicularly to the path of the signals sent by A. That means that *if* B intercepts one signal, then the *next* signal will miss him. So if A is transmitting signals in the y direction, then B is not going to receive more than one signal, and so will be unable to measure any kind of frequency at all. Two ways to rectify this: (1) You can imagine that instead of just one sender, there is an *array* of senders, all sending in the y-direction, all sending in phase. Then if B catches the signal from one sender, he will catch a different signal from a *different* sender. In that case, B will see the signals *BLUESHIFTED*. (2) Instead of A sending in the y-direction, he continually adjusts his signals so that they always reach B. That means he has to aim his signals *ahead* of where B is now. These are *NOT* the same case. In case (2), A is *NOT* transmitting in the y-direction, the angle is changing with time. -- Daryl McCullough Ithaca, NY |
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On Mar 27, 11:28*pm, Koobee Wublee wrote:
On Mar 27, 9:01 am, Daryl McCullough wrote: On Mar 26, Koobee Wublee wrote: What is the transverse Doppler effect under relativity? According to the energy transformation and also your derivation, it should predict a blue shift while experiments time after time all have indicated red. *Oops! *shrug This disagreement of SR with experiments is serious and fatal, no? [So] checkmate Koobee's problem... It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. So, just to recap, what you are saying is that, in your view, the Doppler shift should agree with the derivation that YOU produced and which does NOT agree with experiment, and that on the basis of this result, relativity should be found fault with. Aha. Seto has a similar agenda -- to try to show that relativity says something which it does not say, so that relativity can be discredited. Seto, however, is notoriously stupid, and you have adopted his tactics. ** *f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** *[v] = Velocity vector between frames of f and f ** *[c] = Velocity vector of light ** *[] * [] = dot product of two vectors Under the transverse case, ** *f / f = 1 / sqrt(1 v^2 / c^2) Where ** *[v] * [c] = 0 This means SR predicts a blue Doppler shift in the transverse direction, and that is totally wrong. *shrug Anyone with half a brain would attempt to execute a graceful retreat from that. *shrug It smells like a bunch of sour ass losers with unsportsmanlike conducts. *shrug The bottom line is that SR does not produce what is observed in experiments. *Thus, SR is merely garbage. *Just how difficult can that be? *shrug |
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On Mar 28, 7:50 am, PD wrote:
On Mar 27, 11:28 pm, Koobee Wublee wrote: It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** [v] = Velocity vector between frames of f and f ** [c] = Velocity vector of light ** [] * [] = dot product of two vectors Under the transverse case, ** f / f = 1 / sqrt(1 v^2 / c^2) Where ** [v] * [c] = 0 This means SR predicts a blue Doppler shift in the transverse direction, and that is totally wrong. shrug Anyone with half a brain would attempt to execute a graceful retreat from that. shrug It smells like a bunch of sour ass losers with unsportsmanlike conducts. shrug The bottom line is that SR does not produce what is observed in experiments. Thus, SR is merely garbage. Just how difficult can that be? shrug So, just to recap, what you are saying is that, in your view, the Doppler shift should agree with the derivation that YOU produced and which does NOT agree with experiment, and that on the basis of this result, relativity should be found fault with. OK, lets do a recap. Are the following equations valid under the Lorentz transform and SR? ** f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** [v] = Velocity vector between frames of f and f ** [c] = Velocity vector of light ** [] * [] = dot product of two vectors Under the transverse case, ** f / f = 1 / sqrt(1 v^2 / c^2) Where ** [v] * [c] = 0 If the answer is yes, WTF is the problem? shrug If the answer is no, what do you think is the correct equation describing the transverse Doppler shift under SR? |
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On Mar 28, 3:53 am, Daryl McCullough wrote:
Koobee Wublee says... It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** [v] = Velocity vector between frames of f and f ** [c] = Velocity vector of light ** [] * [] = dot product of two vectors Under the transverse case, ** f / f = 1 / sqrt(1 v^2 / c^2) Where ** [v] * [c] = 0 This means SR predicts a blue Doppler shift in the transverse direction, and that is totally wrong. shrug Anyone with half a brain would attempt to execute a graceful retreat from that. shrug It smells like a bunch of sour ass losers with unsportsmanlike conducts. shrug The bottom line is that SR does not produce what is observed in experiments. Thus, SR is merely garbage. Just how difficult can that be? shrug p_x' = gamma (p_x - Ev/c^2) p_y' = p_y p_z' = p_z E' = gamma (E - p_x v) Is the transverse Doppler equation not the following? ** E' = gamma (E - p_x v) Where ** p_x = 0 If yes, WTF is the problem? The transverse Doppler shift under SR is blue. shrug? If no, what should the correct equation for transverse Doppler shift look like according to you? I don't know why you think that there is some kind of incompatibility. Is the last equation the same as the following? ** E / E = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** [v] = Velocity vector between frames of f and f ** [c] = Velocity vector of light ** [] * [] = dot product of two vectors As yours truly has said, you guys are bunch of sour ass losers. shrug The bottom line is that SR is just garbage. shrug |
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On Mar 28, 9:24*am, Koobee Wublee wrote:
On Mar 28, 7:50 am, PD wrote: On Mar 27, 11:28 pm, Koobee Wublee wrote: It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** *f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** *[v] = Velocity vector between frames of f and f ** *[c] = Velocity vector of light ** *[] * [] = dot product of two vectors Under the transverse case, ** *f / f = 1 / sqrt(1 v^2 / c^2) Where ** *[v] * [c] = 0 This means SR predicts a blue Doppler shift in the transverse *direction, and that is totally wrong. *shrug Anyone with half a brain would attempt to execute a graceful *retreat from that. *shrug It smells like a bunch of sour ass losers with unsportsmanlike *conducts. *shrug The bottom line is that SR does not produce what is observed in experiments. *Thus, SR is merely garbage. *Just how difficult can that be? *shrug So, just to recap, what you are saying is that, in your view, the Doppler shift should agree with the derivation that YOU produced and which does NOT agree with experiment, and that on the basis of this result, relativity should be found fault with. OK, lets do a recap. *Are the following equations valid under the Lorentz transform and SR? ** *f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) You were just given the derivation of the Doppler effect and you just agreed that your derivation is wrong. Yet here we are again. If you don't know what the symbols mean, just ask. Don't just start swapping them around and call it a day. [snip rest, unread] |
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On Mar 27, 10:57 pm, Eric Gisse wrote:
Koobee Wublee wrote: It should be very clear at this stage the Doppler shift no matter how you fudge it to be should agree with the energy transform as described below. ** f / f = (1 + [v] * [c]) / sqrt(1 v^2 / c^2) Where ** [v] = Velocity vector between frames of f and f ** [c] = Velocity vector of light ** [] * [] = dot product of two vectors Its' already been established that you don't know how to derive anything in relativity. What's the point in going over old ground? So, the college dropout thinks the equation above is wrong under SR. shrug You were just given the derivation of the Doppler effect and you just agreed that your derivation is wrong. Yet here we are again. What derivation? Well, the college dropout cannot weasel its way out of this one. Under the transverse case, ** f / f = 1 / sqrt(1 v^2 / c^2) Where ** [v] * [c] = 0 If you don't know what the symbols mean, just ask. Don't just start swapping them around and call it a day. [snip rest, unread] Lets get this straight. The college dropout is bitching about something it has not read. What else is new and expected from a college dropout? shrug |
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