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![]() "Henri Wilson" HW@.... wrote in message ... On 1 Apr 2007 07:57:46 -0700, "George Dishman" wrote: On 26 Mar, 00:56, HW@....(Henri Wilson) wrote: On Sun, 25 Mar 2007 00:31:31 -0000, "George Dishman" wrote: "Henri Wilson" HW@.... wrote in message .. . On Sat, 24 Mar 2007 13:45:26 -0000, "George Dishman" wrote: ... We know the pulsar produces pulses regularly every 2.285ms and it doesn't matter whether that is one or two or 27 per rotation, all that matters is that we can measure that they are emitted with a regularity almost as good as an atomic clock. I was under the imp[ression that the observed pulse was slowly changing too. Not to worry... Pulsars are normally slowing very slightly but it is _very_ gradual: http://outreach.atnf.csiro.au/educat...ryone/pulsars/ "For example, a pulsar called PSR J1603-7202 is known to have a period of 0.0148419520154668 seconds. However the periods of all radio pulsars are increasing extremely slowly. The period of PSR J1603-7202 increases by just 0.0000005 seconds every million years!" ..which is exactly what the BaTh predicts for a pulsar that is in a very large orbit. ..but it is also to be expected that they should be slowing as they lose energy. I see no problem there. "I expect" is not a mathematical prediction. Show the maths that gives you a figure of 500 ns per million years and I'll believe you. The VDoppler contribution is negligible...forget it. Nope, the simple indication from the phase is that it is completely dominant. If you want to forget it you have to show an alternative model, such as a higher eccentricity, that explains the phase. I'm not saying you can't, only that you cannot just wave your hands and pretend the phase data doesn't exist. If you read what I said in tyhe other message you will now know that the VDoppler effect doesn't exist...as I originally thought. We have since corrected that, your new numbers are realistic. The 'correction' is negligible. Fit your model to the observed data. I think you will find it is dominant. I don't really care about that, I want to know why they are delayed after they have been created. Are they delayed or advanced? Ballistic theory says they should be advanced but they are actually delayed. No. The BaTh should be in agreement with GR. It isn't, it ballistic theory predicts an advance, GR predicts a delay. All we have is a theory. It might be completely wrong. How do YOU explain the existence of pulses. The source emits a beam and spins like a lighthouse, you know that already. I don't know that any more. I dont think that explains what is observed. Do you think the beam is a narrowly focussed 'pencil'... or is it a plane? See the illustration here http://outreach.atnf.csiro.au/educat...ryone/pulsars/ In one of the papers I cited some time ago, there was a diagram shoing a cross-section where precession means we have stripes across the beam, like the scan lines of a TV. It's a pretty crappy article. It is not intended as technical. Quote: "The time between pulses, the period, is the time that it takes for the neutron star to rotate once. " Why aren't two pulses emitted per rotation? You are probably thinking of something like the animation on this page: http://science.nasa.gov/newhome/help...als/pulsar.htm In reality, it is probably more like the earlier static picture where the angle between the rotational and magnetic axes is smaller. The second beam is always pointing away from us. and: "Therefore the most likely explanation is that a pulsar is a neutron star that spins rapidly and emits radio waves along its magnetic axis. However, not all neutron stars are necessarily detectable as pulsars. The beams from some neutron stars may never pass the Earth and will therefore not be detected. Also, other neutron stars may have been pulsars in the past, but the process that causes the beam of radiation (which is not fully understood) may have turned off or is just too weak to be detected. " In other words, they don't know. In other words : a) the beams are thin so we expect to see only a fraction of the total number of pulsars. b) the energy to produce the beam runs out eventually. Both pretty obvious really. George, GR and the BaTh have the same equations as regards the slowing of light or the distortion of space to maintain its speed at c. No they don't Henry, nothing like it. George, the BaTh says light speed increases when light falls down a gravitty wwell just like anyhting else does. Yes, so the signals from the pulsar when it is on the far side of the companion should be accelerated towards us and then slowed to the original speed once it has passed the dwarf and is en route to us. That would produce an advance of the arrival time as we discussed some time ago. You appeared to agree the mechanism then so can you go back and have another read, I don't want to write all the same stuff again. GR says the same. No, it predicts a delay. GR effectively says the light s[p]eed remains constant and SPACE contracts to make that so. As the Pound- Rebka experiment showed, both approaches give the same answer. Pound-Rebka showed that processes seem to go slower when viewed from a higher potential. In GR the light seems to move slower when it is close to the companion hence it predicts a delay. But the companion is orbiting the star....not vice versa... Doesn't matter, only the relative speed matters. Move your finger in front of a light or move the light behind your finger and it gets blocked either way. The pulsar is barely moving. You have no model fit that predicts that, it is just handwaving and will turn out to be wrong when you do the work. We see a bright dot in the sky George. It could be anything. No Henry, it could not "be anything", it is a white dwarf because it has the spectrum that falls into that classification. Well if it can be positively identified let''s see its brightness curve. Do you think we can ask someone to try to measure it for us? Are you in touch with any astronomers? No. I suspect they will try to get some telescope time at some point but it will take its place in the priorities. Back to the abuse Henry? I'm just applying Kepler's laws and you say your program uses them so it should agree. Well you got the VDoppler business wrong for a start... Strange how you now agree with me. I agree ..but it is a negligible effect .....and not related to extinction. It is not _related_ to extinction but it allows us to put an upper limit on the distance over which extinction occurs. Fit your model and you'll see what I mean. Theories, theories...all based on wrong data... What is the truth? The truth is that the luminosity drops to near zero for 2 degrees of the orbit, that is the data and it is not an interpretation. eclipses CAN occur. And statistically we expect to see some. There is no reason to think this isn't one and the Shapiro delay matches. ...but there can also be eclipse-like dips in brightness curves caused purely by c+v. But the field rotates hundreds of times a second and the eclipse last 48 seconds every 2.4 hours (figures estimated from memory but right order of magnitude). But what is the form of the magnetic field? How can a magnetic field escape a neutron star when light cannot? Why do you say light cannot escape Henry, of course it escapes or we couldn't receive the pulses. I was under the impression that no light can escape from the neutron star itself. No, that only happens for black holes. In fact we see some pulsars in x-ray and gamma produced by infalling matter hitting the surface. An eclipse isn't hard to interpret. Oh but it is. The Bath expects many orbiting stars to appear as though they are eclipsing. All that is required is a moderately eccentric orbit and a periastron approx. nearest to the observer. Go on then, show how your program produces a drop to zero luninosity, or say by just five or six magnitudes, for just two degrees of the orbit with no variation at any other time. That is what the program is for isn't it? Sure. www.users.bigpond.com/hewn/narrow.jpg Nice. However, don't you get the same shape for the red velocity curve? I think you have used an extreme eccentricity and you are forgetting that the red velocity curve has to be a match to a Keplerian orbit of a much lower value. George |
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On Mon, 2 Apr 2007 22:22:12 +0100, "George Dishman"
wrote: "Henri Wilson" HW@.... wrote in message .. . On 1 Apr 2007 06:46:07 -0700, "George Dishman" wrote: Yes, that's what the observations say they do. What observations george? Are you sugesting that somebody has actually measured the OW speed of individual pulsar pulses wrt Earth? I am pointing out that no observations contradict that view while if ballistic theory was correct you would expect many violations, such as multiple images from binaries. That idea went out the window long ago. You are claiming that as each pulse is emitted, its speed becomes magically adjusted to exactly that of all the previous ones. Nope, and you know pefectly well that's a load of crap Henry, you've been told what SR says far too many times over the years. You are just inventing yet another deliberate distortion to hide from reality. George, you obviously don't even understand your own stupid theory. IT SAYS JUST WHAT I WROTE ABOVE. Don't deny it. Sorry Henry, shouting doesn't make errors any less wrong. I know you are aware of this, I have corrected you on it dozens of times over what must be nearly a decade now. George, SR says that light emitted from differently moving source at the same point will travel through space at the same speed . Are you now denying the very existence of Einstein's second postulate? My original method is 100% OK fall al prcactica purposes. You suggestion is very good and much faster but involves some complicated programming and leaves a lot of gaps in the curve because the x coordinate is rounded off to the nearest integer....and a number of readings may produce the same integer. Still it will work for single stars in most instances. That's often the way, a faster program takes a bit more thought. The choice is yours as to whther the extra complexity is worth the effort. Both methods have advantages and disadvantages. I am trying to include both options in the one program but it's a hell of a job. Speed isn't the key part, remember you said there was no phase shift for zero distance where the VDoppler should dominate so clearly you had a fundamental error. We need to know the phase so your program was unusable at that point. We don't need to know the phase. Yes we do, that is the key as I have been telling you for several weeks, it allows you to distinguish VDoppler from ADoppler which is hard to do any other way unless you are lucky enough to have an eclipsing situation. I have already done that. I gave you the figures. ....but they are just a geometric phenomenon. George, the published 'pulse bunching' curve was used by misguided astrophysicists to determine the velocity curve USING CLASSICAL DOPPLER EQUATIONS. I think they would be using the GR equations Henry. They are effectively the same at low speeds. Yep, but since you emphasised "classical" I thought I should pick that nit. They don't apply...and the figures, upon which the rest of the theory is based, are completely wrong. The theory was written in 1917 Henry, it wasn't based on Hulse and taylor's figures, and the observations exactly match that theory. Yous eem to be getting confused with the Ritzian analysis which would be quite different. SR, LET and BaTh produce almost the same VDoppler shift for speeds c. You should know that. So what, the curve that is matched is the change of the orbit resulting from the energy loss through gravitational radiation. I'm reasonably happy with the idea of energy loss due to a number of factors....although I'm sure matter falling into the pulsar would also slow it down. George, I told you how that can appear to happen. Let me give you a hint Henry, circular orbits don't have a periastron. Well it is probably not exactly circular. maybe e=0.02-04 Fine, you were the one claiming it was circular. I have to compare its curve with a sine wave and look at residuals. . Utter rubbish Henry, the pulse is seen in the radio frequencies below microwave and is a broad band signal, the signals couldn't pulse as fast as they do because the heated gas would cool slowly and the radiation from the disc would be nearly omni-directonal other than some shadowing by other parts of the disc and the star. Well what is YOUR explanation of the pulse origin George? I'm not clear on the details but I understand it to be basically cyclotron radiation in particles pulled from the stellar surface by electrostatic fields. The magnetic field creates the beam by aligning the spiralling of the charges: http://www.sciencedaily.com/releases...0303204842.htm there are many theories George. Nobody really has much of a clue. Maybe, but you don't have the faintest idea how to come up with an alternative that actually explains what we see. 'What we see' is the willusion of what happens. Explaining WHAT IS REALLY HAPPENING is not easy George. It is quite easy Henry, the system emits gravitational radiation exactly as Einstein's maths predicts. Oh crap! As the pope said to allah, "if the faith is strong enough, you can find evidence for it everywhere you look". ![]() Don't you think there might be some degree of magnetic damping? I suggest many possibilities but you never listen. I listen but so far they have all been laughable. They're no funnier than your claim that Einstein's second postulate doesn't really operate even though you have staked your whole reputation on the theory that follows it. YOUR 'sagnac analysis' did nothing more than epitomise the stupidity of trying to use rotating frames of reference. Sixth time now Henry, the analysis you agreed was in the non-rotating frame. Your denial is getting severe, try to calm down a bit. The analysis did not take all factors into account. It was in the non-rotating frame Henry, have you got that now? It took into account all the factors in your diagram. Photon axis, centrifugal force, sideways displacement....etc, etc.... ..and it still showed that a fringe shift should occur. No, it showed there would be _no_ shift. That's why you had to go looking for alternatives. I'm not discussing it futrther here. If you want to stick with the aether explanation then go ahead. There could easily be a local EM FoR that behaves like an aether. No Henry data are the observatory records on which the interpretations are based. So? So you can re-interpret the observations using ballistic theory to produce your predicted orbital parameters but you cannot ignore the data, only the conventional analysis. They measure the bunching of pulses from J1909-3744 and assume it is caused by conventional VDoppler! Which your model will confirm when you do the analysis thoroughly. The analysis IS thorough and it demonstrates my point perfectly. All doppler calculated velocities are likely to be very wrong. Then they arrive at velocities that are grossly exaggerated. Surely you can see that by now. I'm waiting for you to work out what parameters will match the observations. I have given you hints about what the answers will turn out to be but you need to do it yourself, I know you won't believe what I tell you without confirming it for yourself. I've already done it for J1909-3744. For a distance of 3Lys, the (orbital velocity x cos(pitch)) = about 30 m/s. (for a bunching factor, 1 in 10^4) This implies that the pulsar is in a quite small orbit that is somewhat face on. For instance using VDoppler equations to analyse ADoppler bunching of poulasar pulses. Except that ADoppler gives a phase error, that's why the Shapiro effect is important. Where is evidence of this phase error? Where is proof that it is a Shapiro effect? Where is your fit of the ballistic theory model to the observed data? When you do that, the results will be quite clear. We observe the Shapiro effect to coincide with a point of negligible Doppler shift, you want it to be 90 degrees away from where we see it sonow you have stopped talking about the science and started getting abusive instead. Maybe that's a sign that you know subconciously that your claims are unsupportable but I'll give you the benefit of the doubt and wait to see if you can return to the technical discussion. George. I'm not particularly interested in whether or not a Shapiro effect exists because it makes no difference to what my program achieves.. Of course it does Henry, you have to match the phase and Shapiro tells you that So where DOES the supposed Shapiro peak occur? It happens when the LoS passes close to the companion as shown in the diagram: http://www.physorg.com/news9837.html That's 180 out. In the observations, it is at a phase of 0.25 (90 degrees) which is when the Doppler is zero and rising as the source is at its greatest distance from us. See figure 1 of: Where does it say doppler is zero at that point? http://www.arxiv.org/abs/astro-ph/0507420 Theories, theories, George...all based on the wrong velocity figures. I wouldn't believe anything in a paper like this. It's nothing but pure speculation set around statistically manipulated figures. ..the BaTh matching of just about any star curve...and pulsar 'velocity curve'.... Other than your 90 degree phase error of course. I don't have that problem any more. You may be thinking of an older problem of brightness phase relative to velocity which I suspect has been cleared up. Here I mean the observed phase is not compatible with the Doppler being mostly ADoppler, it needs to be predominantly VDoppler. I don't know what the starting phase is in the above figure. I don't understand their phasing at all. Something is 90 out wrt something else yet longitude of periastron (deg) = 155.7452858095 ± 7. What are these two 'somethings'? That in itself isn't a problem, it simply gives an upper limit to the speed equalisation distance. OK, I understand what you are saying but I can't relate it to this figure. George Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On Mon, 2 Apr 2007 22:25:42 +0100, "George Dishman"
wrote: "Henri Wilson" HW@.... wrote in message .. . On Sun, 1 Apr 2007 14:36:54 +0100, "George Dishman" How do we know the orbital phase of a variable star George? Who is talking about variable stars Henry? You suggested I didn't want to look at PSR1613+16 but now you want to change the subject. The theory is that its orbit is highly elliptical and precessing at a known rate. Try to take more care with your terms henry, the theory is GR. That the orbit is elliptical and precessing is the best model fit. If the faith is strong enough George, you will find evidence of it everywhere. I say this pulsar has a nearly circular orbit and maybe its transverse velocity could explain that willusion. Baseless handwaving. I also point out that I don't accept any published astronomical data that is based on grossly wrong values of orbital velocities. Of course not. Produce your best fit of your model to the observations and then we will see whether you agree the rate of orbital change or not. So far you have no evidence to suggest the conventional values are wrong. Stop preaching George and try to understand why Einstein's second postulate requires an aether. George Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On Mon, 2 Apr 2007 22:27:46 +0100, "George Dishman"
wrote: "Henri Wilson" HW@.... wrote in message .. . On Sun, 1 Apr 2007 14:54:22 +0100, "George Dishman" wrote: "Leonard Kellogg" wrote in message egroups.com... Henri Wilson wrote: [grammatical errors corrected to improve readability] Hold a circle (or an ellipse) in front of you at any angle. Rotate your head until you find an axis in the plane of the circle that is horizontal to the line between your eyes, and is also perpendicular to the LOS. (one always exists) ALL the radial velocities and the accelerations around the orbit are then multiplied by the same factor, cos(pitch), where the pitch angle refers to the rotation around the above axis. Rotating one's head is irrelevant. The rotation that you describe (A "roll" of either the head or the projected ellipse) simply puts the long axis of the projected ellipse on the viewer's X axis. That is convienient but has no effect on the process of multiplying radial velocities and accelerations around the orbit by a factor of cos(pitch). You said this previously and I do not understand why George did not point out its irrelevancy at that time. Do I understand your terminology correctly as saying that the "pitch" of an orbit is zero when seen edge-on and 90 degrees when seen face-on? If so, your term "pitch" means the same as "inclination", which is the term everyone else uses in astronomy. Though it is often measured as angular deviation from face-on rather than from edge-on. That is how it is used in arXiv astro-ph/0507420.pdf (Table 1, "Orbital inclination, i") To double-check that we are talking about the same thing, see the illustration of "yaw", "pitch", and "roll" near the top of this page: Leonard, I think Henry has just swapped some definitions for convenience. His cos(pitch) is the same as the usual sin(inclination). I'm less clear about his yaw but I'm fairly sure it is directly related to the longitude of the ascending node. It is the angle between the LOS and the major axis, in the edge on position. Any edge on orbit can be rotated about the axis perpendicular to the LOS. At any particular angle, all RADIAL velocities and accelerations will be multiplied by the same factor, my cos(pitch). ALL POSSIBLE ORBIT CONFIGURATIONS (WRT EARTH) CAN BE CREATED IN THIS WAY. Think about it. I don't need to, I think there is a trivial relationship between your angles and the conventional ones. For example pitch = 90 - inclination I haven't bothered working out the yaw but I'm sure something similar will result. My main point is to show why redefining yaw angle makes it legitimate to use edge-on orbits. Did you try holding up a paper cutout and rotating it around the LOS till you find the axis I talked about? George Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On Mon, 2 Apr 2007 22:29:54 +0100, "OG" wrote:
"Henri Wilson" HW@.... wrote in message .. . On Mon, 2 Apr 2007 19:06:42 +0100, "OG" wrote: Oh what a surprise, HW doesn't respond. Could it be he's wary of reality? Spectral lines don't measure OWLS, idiot. Cut the insults if you want to be taken seriously. Since spectral lines are narrow we know that all the light measured at on time was given off at the same point in the velocity-time cycle. If some light coming from a cepheid was travelling faster than the rest (as you seem to be proposing) we would get broadening of the spectral lines. Poor boy! You're not related to eric geese by any change, are you? So what's your explanation then? Explanation of WHAT? You haven't even described a problem yet. Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On Mon, 2 Apr 2007 22:34:19 +0100, "George Dishman"
wrote: "Henri Wilson" HW@.... wrote in message .. . On Sun, 1 Apr 2007 15:04:46 +0100, "George Dishman" Given that you now accept the huff-puff nature, you need to reconsider your justification for saying that Cepheids that are currently thought of as isolated might actually be part of a binary. Every one I read about seems to have a companion star. Put "solitary cepheid" into Google and you get a number of hits. At least one was a survey listing both categories with similar numbers of entries. I looked it up earlier at work and don't have the reference here and it was in postscript but I'm sure you can find a readable version with a little hunting. I'm sure there are many that have very slow orbit periods. If you are now switching to say they are single stars, why on Earth would your software be modelling binary systems and restricting the solutions to Keplerian orbits when the motion of the surface is due to internal pressure? I think it is my turn to say you are getting very confused Henry. It is a fact that most 'cepheids' appear to have a companion... It is a fact that something around half of _all_ stars are in binary systems so there is no reason why Cepheids should be an exception. ...all stars are obiting some kind of mass centre. They all orbit the galaxy, so what. The orbital period needs to be a few years or less for any significant effects to show up. They orbit all kinds of objects, not just the galaxy...and other objects orbit them. Many orbits will involve more than one other object and will be unstable. It is certainly possible, especially for close binaries, but less likely for those with greater separations. and distorted into some kind of dumbell shape, No, each would be more like an egg shape. Look up "Roche Lobe". Yes, egg shaped...that would cause a brightness variation at double the orbit frequency. leading to a brightness variation as they orbit....but that wouldn't account for the short periods of many of them. It wouldn't account for any where the period of the Cepheid differs from the orbital period, nor does it account for those that are not in binary systems. That is true. That's why I accept the possibility. However it doesn't make any difference to the fact that the brightness variation of huff-puff stars conforms with BaTh. First you need to model them correctly. Your new program should do that if you match the red velocity curve to the published data. The grreen curve then gives the luminosity variation due to c+v and any extra is intrinsic. So Henry, revisit your matches and tell me how much is c+v and how much is intrinsic for some examples 1.5 magnitude variation It isn't difficult to produce variations of 1.5 mag. ..but 3 is about the limit with the BaTh before the critical distance is reached and the curves become peaked. There still appears to be no theory that explains any intrinsic brightness variation of huff-puff stars. In every paper I have read about cepheids, the authors admit the have no theory to link the surface movement to the brightness curve. I won't comment on that without doing some study for myself. George Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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![]() "Henri Wilson" HW@.... wrote in message ... On Mon, 2 Apr 2007 22:29:54 +0100, "OG" wrote: "Henri Wilson" HW@.... wrote in message . .. On Mon, 2 Apr 2007 19:06:42 +0100, "OG" wrote: Oh what a surprise, HW doesn't respond. Could it be he's wary of reality? Spectral lines don't measure OWLS, idiot. Cut the insults if you want to be taken seriously. Since spectral lines are narrow we know that all the light measured at on time was given off at the same point in the velocity-time cycle. If some light coming from a cepheid was travelling faster than the rest (as you seem to be proposing) we would get broadening of the spectral lines. Poor boy! You're not related to eric geese by any change, are you? So what's your explanation then? Explanation of WHAT? You haven't even described a problem yet. You need it spelling out? 1 You seem to argue that the light we see from gas that is moving away from us is coming towards us slower than light from gas that is coming towards us. 2 You also seem to be saying that Cepheid variability is due to 'faster' light catching up with (and adding to the brightness of) slower light as stars move in binary orbits or expand/contract as Cepheids do. 3 Doppler shift - speed of emitting gas towards us or away from us changes the wavelength of the light as we receive it. We can measure the motion of the gas because spectral lines are narrow and the wavelength can be measured precisely. If 2 and 3 are true, then the spectral lines from cepheids _should_ show a range of wavelengths representing the whole spread of speeds from the fastest to the slowest at any one time. This range of speeds would be greatest when the fastest was catching up the slowest (at maximum brightness I assume) 4 However, we do not see broad spectral lines from cepheid variables - hence at any one time the light that we are receiving was all emitted at the same speed relative to us. If you accept 3 and propose 1 to be true, and imply that 2 is a consequence of 1, then observation 4 is a problem for you. |
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On Mon, 2 Apr 2007 22:51:01 +0100, "George Dishman"
wrote: "Henri Wilson" HW@.... wrote in message .. . On 1 Apr 2007 07:57:46 -0700, "George Dishman" wrote: Pulsars are normally slowing very slightly but it is _very_ gradual: http://outreach.atnf.csiro.au/educat...ryone/pulsars/ "For example, a pulsar called PSR J1603-7202 is known to have a period of 0.0148419520154668 seconds. However the periods of all radio pulsars are increasing extremely slowly. The period of PSR J1603-7202 increases by just 0.0000005 seconds every million years!" ..which is exactly what the BaTh predicts for a pulsar that is in a very large orbit. ..but it is also to be expected that they should be slowing as they lose energy. I see no problem there. "I expect" is not a mathematical prediction. Show the maths that gives you a figure of 500 ns per million years and I'll believe you. George if you can tell me how much matter is falling into the star and what is its relative angular momentum, I might be able to provide some kind of answer. You would also have to assume something about magnetic damping and tidal effects due to gaseous atmosphere around it. ..and what is the curvature of its transverse motion? How anyone can seriously claim that it is exactly in line with GR predictions is really funny. The VDoppler contribution is negligible...forget it. Nope, the simple indication from the phase is that it is completely dominant. If you want to forget it you have to show an alternative model, such as a higher eccentricity, that explains the phase. I'm not saying you can't, only that you cannot just wave your hands and pretend the phase data doesn't exist. If you read what I said in tyhe other message you will now know that the VDoppler effect doesn't exist...as I originally thought. We have since corrected that, your new numbers are realistic. The 'correction' is negligible. Fit your model to the observed data. I think you will find it is dominant. I think there is a certain amount of circularity in the logic behind the shapiro delay business. I don't really care about that, I want to know why they are delayed after they have been created. Are they delayed or advanced? Ballistic theory says they should be advanced but they are actually delayed. No. The BaTh should be in agreement with GR. It isn't, it ballistic theory predicts an advance, GR predicts a delay. There is a180 phase difference. How can anyone say which is right? All we have is a theory. It might be completely wrong. How do YOU explain the existence of pulses. The source emits a beam and spins like a lighthouse, you know that already. I don't know that any more. I dont think that explains what is observed. Do you think the beam is a narrowly focussed 'pencil'... or is it a plane? See the illustration here http://outreach.atnf.csiro.au/educat...ryone/pulsars/ In one of the papers I cited some time ago, there was a diagram shoing a cross-section where precession means we have stripes across the beam, like the scan lines of a TV. It's a pretty crappy article. It is not intended as technical. Quote: "The time between pulses, the period, is the time that it takes for the neutron star to rotate once. " Why aren't two pulses emitted per rotation? You are probably thinking of something like the animation on this page: http://science.nasa.gov/newhome/help...als/pulsar.htm Yes. I would expect two pulses per rotation from many pulsars.. I don't even accept that this is the real source of pulses. In reality, it is probably more like the earlier static picture where the angle between the rotational and magnetic axes is smaller. The second beam is always pointing away from us. Maybe..but I would have thought the field is more like a broad plane than a beam. Even the 'magnetic field' idea is an assumption. "Therefore the most likely explanation is that a pulsar is a neutron star that spins rapidly and emits radio waves along its magnetic axis. However, not all neutron stars are necessarily detectable as pulsars. The beams from some neutron stars may never pass the Earth and will therefore not be detected. Also, other neutron stars may have been pulsars in the past, but the process that causes the beam of radiation (which is not fully understood) may have turned off or is just too weak to be detected. " In other words, they don't know. In other words : a) the beams are thin so we expect to see only a fraction of the total number of pulsars. Possibly,..maybe not. b) the energy to produce the beam runs out eventually. It will. Both pretty obvious really. Reasonably. Yes, so the signals from the pulsar when it is on the far side of the companion should be accelerated towards us and then slowed to the original speed once it has passed the dwarf and is en route to us. That would produce an advance of the arrival time as we discussed some time ago. You appeared to agree the mechanism then so can you go back and have another read, I don't want to write all the same stuff again. GR says the same. No, it predicts a delay. Then it has the star's position 180 out...that's all. Pound-Rebka showed that processes seem to go slower when viewed from a higher potential. In GR the light seems to move slower when it is close to the companion hence it predicts a delay. But the companion is orbiting the star....not vice versa... Doesn't matter, only the relative speed matters. Move your finger in front of a light or move the light behind your finger and it gets blocked either way. but it doesn't get blocked in the pulsar. The pulsar is barely moving. You have no model fit that predicts that, it is just handwaving and will turn out to be wrong when you do the work. I gave you some figures. Well if it can be positively identified let''s see its brightness curve. Do you think we can ask someone to try to measure it for us? Are you in touch with any astronomers? No. I suspect they will try to get some telescope time at some point but it will take its place in the priorities. yes. I suppose so. Well you got the VDoppler business wrong for a start... Strange how you now agree with me. I agree ..but it is a negligible effect .....and not related to extinction. It is not _related_ to extinction but it allows us to put an upper limit on the distance over which extinction occurs. Fit your model and you'll see what I mean. ...explain the phasing in diagram1 and I will try. I don't like their method anyway. Theories, theories...all based on wrong data... What is the truth? The truth is that the luminosity drops to near zero for 2 degrees of the orbit, that is the data and it is not an interpretation. eclipses CAN occur. And statistically we expect to see some. There is no reason to think this isn't one and the Shapiro delay matches. Where is evidence of the eclipse? Why do you say light cannot escape Henry, of course it escapes or we couldn't receive the pulses. I was under the impression that no light can escape from the neutron star itself. No, that only happens for black holes. In fact we see some pulsars in x-ray and gamma produced by infalling matter hitting the surface. theories, theories, again George. I'm not saying they are wrong...just suspicious... An eclipse isn't hard to interpret. Oh but it is. The Bath expects many orbiting stars to appear as though they are eclipsing. All that is required is a moderately eccentric orbit and a periastron approx. nearest to the observer. Go on then, show how your program produces a drop to zero luninosity, or say by just five or six magnitudes, for just two degrees of the orbit with no variation at any other time. That is what the program is for isn't it? Sure. www.users.bigpond.com/hewn/narrow.jpg Nice. However, don't you get the same shape for the red velocity curve? I think you have used an extreme eccentricity and you are forgetting that the red velocity curve has to be a match to a Keplerian orbit of a much lower value. Yes...but I hadn't forgotten. I'm trying to find velocity curves for so called eclipsing binaries because they should reveal a great deal about this whole approach. I'm still not convinced that the 'compressible pulse width' method we're using for pulsars applies to light from stars. George Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On 3 Apr, 01:25, HW@....(Henri Wilson) wrote:
On Mon, 2 Apr 2007 22:51:01 +0100, "George Dishman" wrote: "Henri Wilson" HW@.... wrote in message .. . On 1 Apr 2007 07:57:46 -0700, "George Dishman" wrote: Pulsars are normally slowing very slightly but it is _very_ gradual: http://outreach.atnf.csiro.au/educat...ryone/pulsars/ "For example, a pulsar called PSR J1603-7202 is known to have a period of 0.0148419520154668 seconds. However the periods of all radio pulsars are increasing extremely slowly. The period of PSR J1603-7202 increases by just 0.0000005 seconds every million years!" ..which is exactly what the BaTh predicts for a pulsar that is in a very large orbit. ..but it is also to be expected that they should be slowing as they lose energy. I see no problem there. "I expect" is not a mathematical prediction. Show the maths that gives you a figure of 500 ns per million years and I'll believe you. George if you can tell me how much matter is falling into the star and what is its relative angular momentum, I might be able to provide some kind of answer. You would also have to assume something about magnetic damping and tidal effects due to gaseous atmosphere around it. ..and what is the curvature of its transverse motion? How anyone can seriously claim that it is exactly in line with GR predictions is really funny. Nobody claimed it was in line with any GR predictions, you said it was "exactly what the BaTh predicts". If you read what I said in tyhe other message you will now know that the VDoppler effect doesn't exist...as I originally thought. We have since corrected that, your new numbers are realistic. The 'correction' is negligible. Fit your model to the observed data. I think you will find it is dominant. I think there is a certain amount of circularity in the logic behind the shapiro delay business. None at all, just comparison against an empirical curve. Are they delayed or advanced? Ballistic theory says they should be advanced but they are actually delayed. No. The BaTh should be in agreement with GR. It isn't, it ballistic theory predicts an advance, GR predicts a delay. There is a180 phase difference. How can anyone say which is right? What is observed is a delay when the Sun is close to the line of sight to spaecraft and when radar signals are bounced off Venus and so on. There is no question about the observation within the Solar system and both GR and ballistic theory say the effect should be largest when the light passes closest to the body (obviously). The main difference is the sense of the effect. Why aren't two pulses emitted per rotation? You are probably thinking of something like the animation on this page: http://science.nasa.gov/newhome/help...als/pulsar.htm Yes. I would expect two pulses per rotation from many pulsars.. A smaller second pulse half a rotation later is seen from some. I don't even accept that this is the real source of pulses. I don't really care what you accept, all that matters is that pulses are produced and we can use them as a testbed. In reality, it is probably more like the earlier static picture where the angle between the rotational and magnetic axes is smaller. The second beam is always pointing away from us. Maybe..but I would have thought the field is more like a broad plane than a beam. They seem to produce a cone shaped beam or pencil beams, sometimes both. The whole thing is very complex. See section 4 and Figure 2 of http://www.arxiv.org/abs/astro-ph/0407149 Note the signal is low in the centre and highest along the 'hourglass' shaped contour. Even the 'magnetic field' idea is an assumption. There is a lot of evidence backing that up. "Therefore the most likely explanation is that a pulsar is a neutron star that spins rapidly and emits radio waves along its magnetic axis. However, not all neutron stars are necessarily detectable as pulsars. The beams from some neutron stars may never pass the Earth and will therefore not be detected. Also, other neutron stars may have been pulsars in the past, but the process that causes the beam of radiation (which is not fully understood) may have turned off or is just too weak to be detected. " In other words, they don't know. In other words : a) the beams are thin so we expect to see only a fraction of the total number of pulsars. Possibly,..maybe not. Only if all the pulsars in the galaxy happen to point at us. I doubt that. b) the energy to produce the beam runs out eventually. It will. Both pretty obvious really. Reasonably. Yes, so the signals from the pulsar when it is on the far side of the companion should be accelerated towards us and then slowed to the original speed once it has passed the dwarf and is en route to us. That would produce an advance of the arrival time as we discussed some time ago. You appeared to agree the mechanism then so can you go back and have another read, I don't want to write all the same stuff again. GR says the same. No, it predicts a delay. Then it has the star's position 180 out...that's all. We see a delay that peaks like this: _/\_____ An advance shifted by 180 degrees would look like this: _____ _ \/ Not even close. Pound-Rebka showed that processes seem to go slower when viewed from a higher potential. In GR the light seems to move slower when it is close to the companion hence it predicts a delay. But the companion is orbiting the star....not vice versa... Doesn't matter, only the relative speed matters. Move your finger in front of a light or move the light behind your finger and it gets blocked either way. but it doesn't get blocked in the pulsar. One pulsar is blocked by the other. Remember this was discussing the dual pulsar system. The pulsar is barely moving. You have no model fit that predicts that, it is just handwaving and will turn out to be wrong when you do the work. I gave you some figures. Yes, you have looked at a number of test scenarios most of which I asked about to show how they could be eliminated from consideration. What I mean is that you haven't worked through the whole problem to find a single set of numbers that fits all the observational data. It's not a criticism Henry, we just haven't reached that stage yet. Well if it can be positively identified let''s see its brightness curve. Do you think we can ask someone to try to measure it for us? Are you in touch with any astronomers? No. I suspect they will try to get some telescope time at some point but it will take its place in the priorities. yes. I suppose so. Well you got the VDoppler business wrong for a start... Strange how you now agree with me. I agree ..but it is a negligible effect .....and not related to extinction. It is not _related_ to extinction but it allows us to put an upper limit on the distance over which extinction occurs. Fit your model and you'll see what I mean. ..explain the phasing in diagram1 and I will try. As I understand it, the phase is like this: A B + D Earth C A = 0.00 & 1.00 B = 0.25 C = 0.50 D = 0.75 I don't like their method anyway. The terms are fairly standard and you should be able to convert to other angles easily. These should help: http://en.wikipedia.org/wiki/Longitu...ascending_node http://en.wikipedia.org/wiki/Argument_of_periapsis http://www.lns.cornell.edu/~seb/cele...eadsheets.html You might like this too, I came across it by accident http://voyager2.dvc.edu/faculty/kcas...tar%20Dat3.htm There's a bit of a glossary at the bottom. Theories, theories...all based on wrong data... What is the truth? The truth is that the luminosity drops to near zero for 2 degrees of the orbit, that is the data and it is not an interpretation. eclipses CAN occur. And statistically we expect to see some. There is no reason to think this isn't one and the Shapiro delay matches. Where is evidence of the eclipse? The fact that the flux dips to near zero coincident with the Shapiro delay maximum, point B on the above diagram. Why do you say light cannot escape Henry, of course it escapes or we couldn't receive the pulses. I was under the impression that no light can escape from the neutron star itself. No, that only happens for black holes. In fact we see some pulsars in x-ray and gamma produced by infalling matter hitting the surface. theories, theories, again George. No Henry interpretations. You really should know what the word "theory" means by now and not be using it like a layman. I'm not saying they are wrong...just suspicious... These are all areas of on-going research but it is a fact that we see X-ray and gamma emissions and I believe the spctra can give some indication of the surface composition. Anyway, there is no reason why we shouldn't see the surface, the free-fall speed would be about half the speed of light so there would be _significant_ gravitational redshift. Go on then, show how your program produces a drop to zero luninosity, or say by just five or six magnitudes, for just two degrees of the orbit with no variation at any other time. That is what the program is for isn't it? Sure. www.users.bigpond.com/hewn/narrow.jpg Nice. However, don't you get the same shape for the red velocity curve? I think you have used an extreme eccentricity and you are forgetting that the red velocity curve has to be a match to a Keplerian orbit of a much lower value. Yes...but I hadn't forgotten. I'm trying to find velocity curves for so called eclipsing binaries because they should reveal a great deal about this whole approach. I'm still not convinced that the 'compressible pulse width' method we're using for pulsars applies to light from stars. I am discussing J0737-3039 which is a double pulsar system with an eclipse. The velocity curve should be easy to find or perhaps figure out from the orbital elements (as before work back using conventional theory to find the observations thenre-interpret using ballistic theory). George |
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On Tue, 3 Apr 2007 01:23:35 +0100, "OG" wrote:
"Henri Wilson" HW@.... wrote in message .. . On Mon, 2 Apr 2007 22:29:54 +0100, "OG" wrote: Poor boy! You're not related to eric geese by any change, are you? So what's your explanation then? Explanation of WHAT? You haven't even described a problem yet. You need it spelling out? 1 You seem to argue that the light we see from gas that is moving away from us is coming towards us slower than light from gas that is coming towards us. That's correct. Light moves at c wrt its source and c+v wrt us. 2 You also seem to be saying that Cepheid variability is due to 'faster' light catching up with (and adding to the brightness of) slower light as stars move in binary orbits or expand/contract as Cepheids do. Well the light curves match perfectly...that's alI can produce as evidence.. 3 Doppler shift - speed of emitting gas towards us or away from us changes the wavelength of the light as we receive it. We can measure the motion of the gas because spectral lines are narrow and the wavelength can be measured precisely. According to BaTh, the frequency of arrival of 'wavecrests' varies with incoming light speed. The BaTh doppler equation is virtually the same as those of SR and LET for vc. If 2 and 3 are true, then the spectral lines from cepheids _should_ show a range of wavelengths representing the whole spread of speeds from the fastest to the slowest at any one time. This range of speeds would be greatest when the fastest was catching up the slowest (at maximum brightness I assume) This is not true. It is apparent that no 'fast light' ever catches the slower light because of extinction. For cepheids, a range should be observed because the spherical surface will be expanding at different rates accros the disk. 4 However, we do not see broad spectral lines from cepheid variables - hence at any one time the light that we are receiving was all emitted at the same speed relative to us. You WOULD EXPECT to see broadened lines from huff-puff cepheids for the above reason. If they are narrow, then it backs up the BaTh and the theory that they are really just ordinary stars in orbit.. If you accept 3 and propose 1 to be true, and imply that 2 is a consequence of 1, then observation 4 is a problem for you. Thankyou Og for backing up the BaTh and shooting yourself in the foot. Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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