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![]() "Henri Wilson" HW@.... wrote in message ... 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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On 3 Apr 2007 07:02:49 -0700, "George Dishman"
wrote: 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 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". That paper you referred me to claimed it was. 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. George, the BaTh says all light leaving the pair will be slowed slightly, causing an overall redshift that may or may not be counterbalanced by the blue shift arising from its accelerated approach to our galaxy and Earth. When the star is on the near side, the bending of light by the dwarf more than compensates for the increase in average light speed. So The BaTh says that there should be a shapiro type slowing. 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. yes. 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. Fair enough...but the distance of their origin from the pulsar could be important for the BaTh. 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. Yes. Even the 'magnetic field' idea is an assumption. There is a lot of evidence backing that up. It could for instance be a beam of radiation that excites surounding gas.. Anyway I suppose it doesn't matter much for our purposes. "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. No. The BaTh expects the same kind of delay due to bending and increased light path lengths. I was wrong about the 180 difference. 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. I'm a bit confused as to which pulsar we are discussing now. 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 you see I don't use this convention. My pitch is not quite the same as their inclination because I rotate my head around the LOS until the line joining the yellow and grey sections is perpendicular to the LOS. Such a line can always be found....for any orbit. The ecliptic plane is simply rotated. Having done that, their 'longitude of ascending node' becomes my yaw angle. http://en.wikipedia.org/wiki/Argument_of_periapsis http://www.lns.cornell.edu/~seb/cele...eadsheets.html All these angles are irrelevant in my method. You might like this too, I came across it by accident http://voyager2.dvc.edu/faculty/kcas...tar%20Dat3.htm Yes I found that one some time ago. I already matched one of the curves there. 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. Is this still with reference to the dual pulsar system? If so there should be two Shapiro effects per cycle. 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. So what is the actual doppler shift of the EM that makes up the actual pulses of a neutron star? It should be very heavily redshifted and the pulses should start out at maybe c/2. ...this is why I don't believe the pulses are actually produced near the pulsar itself but at a considerable distance away. 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). I'll see what I can find. George Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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![]() "Henri Wilson" HW@.... wrote in message ... 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. What is BaTh? 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. That's convenient - you had better explain 'extinction and why it only affects some light and not all of it For cepheids, a range should be observed because the spherical surface will be expanding at different rates accros the disk. Agreed, but the profile will be modulated as the sine of the cepheid's surface so that majority of the light emitted will be relatively close to the actual surface velocity. The shape of a spectral line is known and explained. 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. See the above. If they are narrow, then it backs up the BaTh and the theory that they are really just ordinary stars in orbit.. No because you haven't explained 'extinction' Nor does it explain why different elements have different velocity profiles across the light curve. 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. On the contrary - you need to explain yourself So 3 questions What is BaTh ? What is extinction and how precisely does it prevent fast light from catching up slow light? What is your explanation for the variable light curve of cepheids I'm away from fast internet for the next few days so you can take your time over these answers. |
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On Apr 3, 5:07 pm, HW@....(Henri Wilson) wrote:
On Tue, 3 Apr 2007 01:23:35 +0100, "OG" wrote: 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 consequenceof 1, then observation 4 is a problem for you. Thankyou Og for backing up the BaTh and shooting yourself in the foot. Actually, Henri, you've just shot YOURSELF in the foot. Periodic broadening and narrowing of the spectral lines of Cepheids is a well documented phenomenon. This periodic Doppler broadening results from three phenomena operating concurrently: 1) Projection effect. The parts of the photosphere pulsating in our line of sight show greater Doppler shift than the parts of the photosphere which are pulsating tangentially with respect to us. 2) Thermal effect. Doppler broadening due to kinetic effects varies as the Cepheid heats and cools through its cycle. 3) Turbulence effect. Spectral lines show periodic Doppler broadening as the Cepheid "boils up" and relaxes. Here is a good reference for you to read. http://www.obs-hp.fr/www/preprints/pp119/pp119.html BaTh fails yet again!!!!! Jerry |
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On 3 Apr 2007 17:19:13 -0700, "Jerry" wrote:
On Apr 3, 5:07 pm, HW@....(Henri Wilson) wrote: On Tue, 3 Apr 2007 01:23:35 +0100, "OG" wrote: 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 consequenceof 1, then observation 4 is a problem for you. Thankyou Og for backing up the BaTh and shooting yourself in the foot. Actually, Henri, you've just shot YOURSELF in the foot. Periodic broadening and narrowing of the spectral lines of Cepheids is a well documented phenomenon. This periodic Doppler broadening results from three phenomena operating concurrently: 1) Projection effect. The parts of the photosphere pulsating in our line of sight show greater Doppler shift than the parts of the photosphere which are pulsating tangentially with respect to us. 2) Thermal effect. Doppler broadening due to kinetic effects varies as the Cepheid heats and cools through its cycle. 3) Turbulence effect. Spectral lines show periodic Doppler broadening as the Cepheid "boils up" and relaxes. Here is a good reference for you to read. http://www.obs-hp.fr/www/preprints/pp119/pp119.html BaTh fails yet again!!!!! Where did I disagree with any of the above....? I suggest you go back to sticking needles in dead bodies... Jerry Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On Wed, 4 Apr 2007 00:28:34 +0100, "OG" wrote:
"Henri Wilson" HW@.... wrote in message .. . 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. What is BaTh? 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. That's convenient - you had better explain 'extinction and why it only affects some light and not all of it For cepheids, a range should be observed because the spherical surface will be expanding at different rates accros the disk. Agreed, but the profile will be modulated as the sine of the cepheid's surface so that majority of the light emitted will be relatively close to the actual surface velocity. The shape of a spectral line is known and explained. 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. See the above. If they are narrow, then it backs up the BaTh and the theory that they are really just ordinary stars in orbit.. No because you haven't explained 'extinction' Nor does it explain why different elements have different velocity profiles across the light curve. 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. On the contrary - you need to explain yourself So 3 questions What is BaTh ? What is extinction and how precisely does it prevent fast light from catching up slow light? What is your explanation for the variable light curve of cepheids I'm away from fast internet for the next few days so you can take your time over these answers. Why should I bother to answer at all? Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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On Apr 3, 10:09 pm, HW@....(Henri Wilson) wrote:
On 3 Apr 2007 17:19:13 -0700, "Jerry" wrote: BaTh fails yet again!!!!! Where did I disagree with any of the above....? So you admit it! BaTh fails EVERY test! Jerry |
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On 4 Apr, 00:17, HW@....(Henri Wilson) wrote:
On 3 Apr 2007 07:02:49 -0700, "George Dishman" wrote: 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 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". That paper you referred me to claimed it was. I'm surprised but I don't have that one handy. Are you sure you aren't thinking of the Hulse and Taylor paper? Pulsar rate slowing is due to the magnetic field and I don't think GR even comes into it, nor does ballistic theory AFAICS. 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. George, the BaTh says all light leaving the pair will be slowed slightly, causing an overall redshift that may or may not be counterbalanced by the blue shift arising from its accelerated approach to our galaxy and Earth. Henry, have a look at the earlier message in this thread where we discussed this: http://groups.google.co.uk/group/sci...3b2a017ef89b9b Your conclusion was: Right so the signal arrives earlier, it is not a delay. The gravitational redshift is identical in each case as is the eventual speed. that's right. When the star is on the near side, the bending of light by the dwarf more than compensates for the increase in average light speed. So The BaTh says that there should be a shapiro type slowing. Let's see the maths Henry. If you are right then you can add that curve to you program and then we will see if you can really match the curves. 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. Fair enough...but the distance of their origin from the pulsar could be important for the BaTh. I doubt it unless it was well outside the binary system but then there would be little variation in any of the parameters. 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. Yes. Even the 'magnetic field' idea is an assumption. There is a lot of evidence backing that up. It could for instance be a beam of radiation that excites surounding gas.. No, the excitation would take far too long to decay and the pulse would probably have a longer tail. Anyway I suppose it doesn't matter much for our purposes. Not really. 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. No. The BaTh expects the same kind of delay due to bending and increased light path lengths. I was wrong about the 180 difference. OK, so now show me the maths you used to find that there is an overal delay. 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. I'm a bit confused as to which pulsar we are discussing now. The history is lost in the snipping but different bits of the post refer to different systems. The eclipsing system is J0737-3039 which is two pulsars. ..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 you see I don't use this convention. Maybe not but you need to understand it if you want to know what a longitude of periastron of 155 degrees means in your terms. .... 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. Is this still with reference to the dual pulsar system? Yes. If so there should be two Shapiro effects per cycle. There should but the pulses from the second pulsar are very hard to detect. They have only recently caught them for a small part of the orbit. Again, being a thin beam there is a finite chance that it won't sweep over us. Now that it has been found there might be a more extensive study in the future. 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. So what is the actual doppler shift of the EM that makes up the actual pulses of a neutron star? It should be very heavily redshifted .. AFAIK it is a continuum with no lines to be measured. Remember we are talking about radio signals in the VHF to microwave bands. and the pulses should start out at maybe c/2. ...this is why I don't believe the pulses are actually produced near the pulsar itself but at a considerable distance away. The slow initial speed would just give an overall distance value that is higher than actual, but only by a few light hours at most and we don't know the distance better than tens of light years, and since the error would be constant, it doesn't have any effect we can measure. 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 then re-interpret using ballistic theory). I'll see what I can find. OK. If you can add a curve for the ballistic theory Shapiro effect, then we can really see how well you can match the observations. George |
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On 3 Apr 2007 21:57:53 -0700, "Jerry" wrote:
On Apr 3, 10:09 pm, HW@....(Henri Wilson) wrote: On 3 Apr 2007 17:19:13 -0700, "Jerry" wrote: BaTh fails yet again!!!!! Where did I disagree with any of the above....? So you admit it! BaTh fails EVERY test! Silly lttle girl..! Jerry Einstein's Relativity - the greatest HOAX since jesus christ's mother. |
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![]() "Henri Wilson" HW@.... wrote in message ... On Wed, 4 Apr 2007 00:28:34 +0100, "OG" wrote: On the contrary - you need to explain yourself So 3 questions What is BaTh ? What is extinction and how precisely does it prevent fast light from catching up slow light? What is your explanation for the variable light curve of cepheids I'm away from fast internet for the next few days so you can take your time over these answers. Why should I bother to answer at all? No reason - if you don't want to support your claims, I can't force you to. You are in the position of wanting to promote your hypothesis, if you don't want to support it . . . |
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