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George Dishman wrote in message
... A minor correction and a bit more on "local". "George Dishman" wrote in message ... "greywolf42" wrote in message ... George Dishman wrote in message ... {A correction to earlier post} Ned's page assumes the temperature at the time of emission was 2.998K. the material that emitted that radiation, a thin shell at a distance of about 420MPc (0.1 * 4.2GPc) is still there. I guessed the difference between linear and exponential wouldn't be too great at 0.1 but it is more than I expected. 4200GPc * ln(1.1) = 400MPc Rather than retype this, can you replace "420MPc" by "400MPc" where appropriate. ------------------------------------- {The starlight-localized issue} That doesn't tell me why you claim that starlight energy would be localized. There seems to be some confusion, you were the one who said the CMBR was locally generated. I would have assumed for your description that it would be the intergral of the electron radiation reduced by tired light hence exponentially decreasing with a characteristic length of over 4GPc. ??? The CMBR is not starlight. You still haven't let me know why you think that starlight energy would be "localized." I don't think it would be localised. Thinking back, I did argue this although .. Then I think we can drop it. _You_ said the CMBR was generated within tens of parsecs ... that is also true, so let me clarify. You said a couple of posts back: "greywolf42" wrote in message ... Light waves return a given fraction of their energy and momentum into the aether (or whatever is assumed by the specific tired light theory). Regardless of source. The "returning" is a local effect (at the point of fractional return). dE = - const E, at the point of inspection. The energy removed by tired light reduces over GPc distances so at short range is negligible. The energy per unit volume from a star then varies as the inverse square of the distance from the source Light energy from a star drops off below the inverse square distance law in the tired light model. so we should see a higher CMBR temperature looking along a line of sight that passes near to a star. No, because your starting assumption was wrong. I argued that we don't see this. I don't know of any reason that we should. The same applies at greater distances if we look along a line that passes close to, but not through a distant galaxy. Again this is not observed so conflicts with the suggestion that the source is illuminated in this way. Now I'm quite willing to believe I have simply not understood your model, but you need to explain this point if I am to understand. Explanation provided above. Your hand-wave (unquantified) argument was based on a bad assumption. In other areas however, you have said that the aether is at a uniform temperature. I've said that we don't expect it to be heated in the local region of stars. It is roughly uniform. We can apply the test on Prof. Wright's page to your theory No, we cannot. Because Ned's page assumes that temperature decreases with time; as a result of BB expansion. Temperature does not change with time in tired light theory. If we take your version of what Ned's trying to do, Ned's curves are trivially incorrect. and find out whether it holds up but obviously you need to tell me the spatial and temporal variation of the temperature (or more accurately the emitted radiation spectrum) before we can do that. I've repeatedly given you that. There is no significant change in temperature with distance and time. As I've said before, I haven't seen anyone propose a tired light theory that would survive that test but maybe you'll be the first. Completely disingenuous. Because you've never looked at a *real* tired light theory. Only Ned's strawmen compton scattering theories. Which is the purpose of strawmen, of course. -- greywolf42 ubi dubium ibi libertas {remove planet for return e-mail} |
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George Dishman wrote in message
... Much snipped to try to get back to the physics. "greywolf42" wrote in message ... George Dishman wrote in message ... "greywolf42" wrote in message m... snip The point is, that tired light theoreticians usually don't require that *ALL* the redshift be due to tired light. We try to avoid the trap that caught the big bangers. Next you seem to go back on this but I don't think it's important at present. snip stuff resulting from my typo Tired light AIUI is suggested to explain only the large scale variation with distance. Obviously gravitational redshift and Doppler due to proper motion add to this. If you are now introducing another factor perhaps you could explain the details. I am not attempting to introduce another factor. I believe we agree that gravitational redshifts and "true" doppler shifts (from real velocity differences, not cosmological expansion) are not a factor in tired light theories. We have to allow for them in some fashion, but they aren't central to the theory. Above you said that not all the red shift needed to be due to tired light and suggested this was different from BB. Yes. I agree that gravitational and proper motion effects are present as well but that applies to BB too so what did you mean above? That the BB considers all redshift to be due to doppler due to expansion -- with miniscule corrections from peculiar motion dopplers and gravitational shifts. The BB acknowledges that gravitational redshift, *real* motion dopplers, and electron scattering do exist. But they are only minor corrections on the whole. Tired light theories presume the *additional* source of "tired light", from photon energy degradation. But tired light theories therefore consider that (non-expansion) doppler effects from "peculiar" or systematic motions will not simply be small corrections to the cosmic expansion signature. Tired light theories agree with the BB that gravitational redshift and electron scattering will be minor corrections on the whole. All the above say that it should be exponential in theory, but what we are asking is how you turn that into the claim that the exponential has been observed as a result of the paper you cited. I thought you and Bjoern were being deliberately obtuse, and implying that you didn't understand how luminosity (magnitude) could be considered distance. I was specifically addressing your statement: "what is observed is redshift versus magnitude or some other indirect measure of distance." Magnitude is an indirect measure of distance (since the days of Wirtz and Hubble). So, we have a curve of redshift vs. distance. And the observed curve is exponential. At least within error bars. As I said to Bjoern, I didn't want to get another topic going in this thread. I've asked the question and you've given an answer so I'll leave it to him to pick this up if he wishes. Using your data, above, dE/E is about 0.024% per MPc. And every photon loses about 63% of its energy every 4.2GPc. Actually that is now wrong if you are saying that part of the redshift is due to "plasma fireworks", "expanding galaxies" or whatever. How does the 0.024% split between tired light and these other mechanisms? That's why I said I'd work with your numbers. Let's keep it simple. One does not need to have all the answers at the beginning..... OK, that will let me illustrate how I think Ned's test applies. I'll essentially throw a strawman at you and you can then correct the errors in my understanding of your model and we will see if that solves the problem. Just doing the best you can with your view of Ned's site will be fine. But use a *real* tired light theory. (i.e. Vigiers.) I have no desire to deal with yet another strawman. -- greywolf42 ubi dubium ibi libertas {remove planet for return e-mail} |
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Joseph Lazio wrote in message
... "g" == greywolf42 writes: g Joseph Lazio wrote in message g ... g "Dark energy" was not predicted by the big bang. Dark energy is an g ad hoc modification to the BB, to explain a deviation between the g form of the observed redshift-distance curve versus the theoretical g redshift-distance curve. The form of the observed g redshift-distance curve was predicted by tired light. Recall that Einstein inserted the cosmological constant because, at the time he developed general relativity, everybody "knew" the Universe to be static. After Hubble's discovery, [...] there was no observational basis for the cosmological constant, so it was reasonable to set its value to 0. Once sufficient evidence for a non-zero value accumulated, people were quite happy to include it. "Dark energy" is just the fancy modern name given to the cosmological constant because it has since been realized that the cosmological constant might not be constant. g Dark Energy was the name given because Cosmologists had thrown out g Einstein's cosmological constant ... not just set it to zero (or, g more precisely, unknown). Hence, when the SN1a data arrived, they g couldn't think outside their pet paradigm. And simply added g another epicycle. You persist in asserting that dark energy is somehow radically different than the cosmological constant I never made any such claim. Or any similar claim. and that the cosmological constant was never considered by astronomers I never made any such claim. Or any similar claim. and is somehow not part of general relativity. This is a claim I did make. Take a look at Einstein 1915-16. No cosmological constant. The CC is part of Relativistic Cosmology (1918-19). It is not part of GR. Relativistic cosmology *includes* GR, but it is not *only* GR. GR is part of Relativistic Cosmology. Could you provide some citations for these views? Use google. I've provided the responses many times. If you provide a link to any specific claim that I've actually made (instead of your trolling falsehoods, above), I'll provide you with the link to the response. -- greywolf42 ubi dubium ibi libertas {remove planet for return e-mail} |
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Joseph Lazio wrote in message
... "g" == greywolf42 writes: g Greg Hennessy wrote in message g ... You mean the one where the values for Ho are around 60-70, about what WMAP shows? g I mean the one that didn't match observations, of course. Greg has covered many of these points quite well. I'll just point out that a quick literature search reveals over 200 papers containing "SZ effect" in their abstracts. I'm sure that the number would probably double were I to also search with the names spelled out. Marvellous. But number of hits on a literature search tells us nothing about the content of the papers. No doubt all of these papers will be dismissed because none of the hundreds of people who have worked on the observations of the SZ effect realized the "circularity" of their noise measurements. I don't dismiss papers without reading them. On the other hand, I don't accept the results of papers without reading them. Especially when someone starts counting without reading. -- greywolf42 ubi dubium ibi libertas {remove planet for return e-mail} |
#115
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The majority of this reply addresses Ned Wright's page.
I'll deal with a tired light test in my other reply to try to focus each branch of the thread. I'm hoping this one can die soon. "greywolf42" wrote in message ... George Dishman wrote in message ... "greywolf42" wrote in message ... George Dishman wrote in message ... snip I've already repeatedly shown where you've misunderstood real tired light theories, and why the test isn't applicable. You insist on examining only strawman theories. The test isn't applicable, because Ned's "test" assumes CMBR temperature reduction from the BB cosmogenesis. And I've repeatedly pointed out that there is no temperature change implied or assumed. I'll snip some further comments based on this misunderstanding. snip I want you to respond to what _I_ am writing. I am responding to what you are writing. You keep writing about Ned's page, and Ned's test. Therefore, I must address Ned's page, and Ned's test. And you claimed "you need to apply it to a specific theory to find out whether it can falsify it or not". If you really believe that Ned needs to change his site to reflect this view, why not say so? There is nothing wrong with Ned's page for what it tries to do IMO. YMMV. Nope. It can only be applied by assuming that the BB is correct, and the temperature that Ned arbitrarily selected (solely to impugn the actual theories) came from the BB. Wrong, it comes from choosing an arbirtrary figure of z=0.1 and choosing the temperature to match the peak wavelength after tired light is applied. The intensity then follows. Well, this *is* a different rationale than Ned provided. Thank you. That's all I meant by listening to my view. However, this can't be true for Ned's curves. Because the intensity between Ned's blue and red curves is unchanged. Photon frequency lowers in a tired light model, *because* energy is lost. Yet Ned's red curve shows energy per photon as unchanged after (you claim) tired light shifting has taken place. It appears that when you include the energy loss, the red curve once again drops to the black (observed) curve. Note that the Y scale is in M Jy / sr. 1 Jansky is 10^-26 watts per square meter per Hz. The "per Hz" factor compensates for this because an interval of 1Hz at the receiver started out as 1.1Hz at the source. Tired light effectively compresses the power emitted into a narrower band. snip So are you saying that the CMBR isn't produced within tens of parsecs? I would assume it was the integral of contributions over many GPc That *IS* the BB assumption, again. No, I mean that it will be a number of times the characteristic length we worked out for tired light, i.e. several times 4.2GPc. unless extinction plays a significant part. You need to tell me over what range extinction becomes important if we are to move forward. I have no need to feed your attempts to throw random objections around. At the moment, we are discussing Ned's argument. Or your version of it. Please do so, or drop it. Fine, but don't complain later that my argument is flawed because I didn't take extinction into account. small snip - moved later big snip Let me make it simple, is the temperature of the aether constant, falling or rising in your model, or doing something else I haven't thought of? As repeatedly noted, it is approximately constant with time. Which is why I favor it. See the very next statement of my post: OK, that's fine. (Your next statement didn't address the time variation of the temperature.) I assume there is a contribution from EM pasing through, which includes both ambient starlight and the CMBR itself. However the effect is not to remove photons as in extinction but just to reduce their energy creating the tired light effect. That is my favorite assumption at the moment. However, there is no a priori need for such an assumption. There is a need to have a specific model to work with if you want specific comments. Otherwise all you can get is hand-waving. We agree then, that Ned's page is merely hand-waving. For he attempts to address all tired light theories with his claims. But Ned doesn't actually address even one single, specific model. No, it is not handwaving. It is an accurate quantitaive explanation of a test that can be applied but you need to know the details of the theory before applying it. snip Ned's source is at 420MPc which I can understand would be non-local by normal standards, but could be 'local' by cosmological standards. Where do you want to draw the line? snip 3) The local region for the MMBR (measured microwave background radiation) is the antenna of the device you are using. According to the matter theory that I favor. If you are suggesting the instrument designers didn't consider locally generated thermal noise in the receiver, that is obvious nonsense. It is a major problem and has to be designed for, tested and calibrated. Ned's model is at a single temperature. Time variation of that temperature is of no relevance to the argument. Ned's model is at a temperature of 2.998 K at emission (time #1) and a temperature of 2.73 at reception (time #2). section snipped from above At a temperature of 2.998 K, instead of the 2.73 K measured "here". That *IS* two different temperatures at two different locations (420 MPc apart). ... It's as if you were additionally assuming that the temperature was 2.725K now as well as 2.998K at the time of emission. That's what Ned's graph is based upon -- This is where you are making your mistake. The page is based on one fact, that the temperature measured here and now is 2.725K. As an example, he then considers the postulate that it was emitted at 2.998K at a distance of 400MPc and the peak has been moved by tired light to coincide with the peak frequency of a black body of 2.725K. There is no suggestion that the actual source is at 2.725K at any time. aside from being an obviously incorrect calculation. See above, the units are not what you thought. snip ONLY big bang theory requires the temperature to change with time. No change with time is implied, in the example it is a source at constant temperature of 2.998K at z=0.1 The time used by Ned is the time it takes for light to travel from z=0.1. That's where he got the temperature (the BB). Wrong, he got it from by back-calculating from the current observed temperature, and you already said that. Then why did you say "wrong?" Because you said "The time used by Ned" suggesting there is a time variation involved. There isn't, only the shift of peak frequency due to tired light acting over a distance. If the distant source is still at that temperature, in the future we will continue to see the CMBR at the same temperature as at present. This is a spurious argument. For we can only measure the present. I hope you now follow the above comment. Your model has the temperature as constant so the measured spectrum would also be constant in time. No, it only assumes the temperature was 2.998K at the time and location of emission. Which is a slowly falling temperature. You aren't dumb. Tell me, why do you feel the need to make excuses for Ned's slime site? Because you are making an incorrect assumption that means you fail to understand the test. I intend to apply the same test but to your distributed source which is at uniform temperature so you need to open your mind a bit and take the blinkers off. To what "distributed source" are you referring? I think you are again looking at nonlocal sources. I thought you said the CMBR was emitted by electrons being excited by the aether, though now you seem to be claiming that the people who designed COBE, WMAP and all the other instruments that have measured the CMBR can't tell the difference between the CMBR and thermal noise in the instrument. If that's your best alternative to the big bang, I don't think much of it! snip He doesn't, you need to re-appraise the page. Not based on Ned's writings. *You* have come up with a different rationalization than Ned states. However, your reasoning does not support Ned's graph. (Or vice versa.) snip That's what I intend to disprove, but you have to get rid of your preconceptions and start thinking about the physics instead. The classic ad hominem. If you intend to disprove it, feel free. It was not intended as an insult of any form, above you say my view differs from Ned's and that suggests you have considered my words separately which is all I wanted. within the posted error bars." In short, only theories with changing temperature of space (specifically those that use the BB rate-of-change) have a problem with Ned's false assertions in the first place. There is no reason to expect a change of temperature ... except in the BB. I think you will eventally start arguing the opposite of that, but see what comes. Nonsubstantive, ad hominem. Again that was not an insult, just an expectation of where the physics will lead us. Sigh. Extinction due to grey dust is not contained in any tired light theory. Only in strawmen. Hence I frankly don't care to go out on another tangent. That's fine. That means I don't need to worry about including what-if's to cover it. It'll make the discussion easier. George |
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References lost due to ISP problem.
"greywolf42" wrote in message ... George Dishman wrote in message ... snip Above you said that not all the red shift needed to be due to tired light and suggested this was different from BB. Yes. I agree that gravitational and proper motion effects are present as well but that applies to BB too so what did you mean above? That the BB considers all redshift to be due to doppler due to xpansion -- with miniscule corrections from peculiar motion dopplers and gravitational shifts. The BB acknowledges that gravitational redshift, *real* motion dopplers, and electron scattering do exist. But they are only minor corrections on the whole. Laying aside gravitational and other secondary effects (S-Z etc.), the essential difference is that expansion deals with the systematic motion while proper motion is essentially that which departs from the overall trend. Tired light theories presume the *additional* source of "tired light", from photon energy degradation. Yep, got that. But tired light theories therefore consider that (non-expansion) doppler effects from "peculiar" or systematic motions will not simply be small corrections to the cosmic expansion signature. I still don't see the difference. To take a crude example, the motions of individual galaxies in a cluster relative to the centre of momentum would be proper motion while that of the CoM itself would be mainly expansion but with an equivalent proper motion relative to neighbouring clusters. Is that not the same in both views? Any systematic outward motion that would contribute to the first order coefficient is simply expansion so you seem to be suggesting that tired light could include an element of expansion. Subtracting the tired light part would then give you still a big bang model but with a much greater age. To avoid a big bang scenario, you need to explain all the systematic red shift with something other than motion and at the moment I'll have to take that as photon energy loss unless you can identify another contributor. Tired light theories agree with the BB that gravitational redshift and electron scattering will be minor corrections on the whole. Yes, I think those are common. OK, that will let me illustrate how I think Ned's test applies. I'll essentially throw a strawman at you and you can then correct the errors in my understanding of your model and we will see if that solves the problem. Just doing the best you can with your view of Ned's site will be fine. But use a *real* tired light theory. (i.e. Vigiers.) I have no desire to deal with yet another strawman. I'll ask you about your view. If that includes elements of Vigiers then fine but if you want to make the case that a tired light theory can satisfy the tests, it is for you to make that case. George |
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George Dishman wrote:
Much snipped to try to get back to the physics. "greywolf42" wrote in message ... (replying to greywolf here, not to George...) [snip] I thought you and Bjoern were being deliberately obtuse, Well, that's one of the big problems when discussing with you: that you constantly invent motives for your discussion partners, instead of actually trying to understand what they are asking and saying. And yes, this is indeed an ad hominem. An eye for an eye... and implying that you didn't understand how luminosity (magnitude) could be considered distance. I was specifically addressing your statement: "what is observed is redshift versus magnitude or some other indirect measure of distance." Magnitude is an indirect measure of distance (since the days of Wirtz and Hubble). So, we have a curve of redshift vs. distance. Yes, we can indeed get such a curve from the luminosity-redshift curve in the reference you gave. And the observed curve is exponential. I don't think so. Where do you get this from? At least within error bars. If you think so: Care to test if an exponential curve, or the curve predicted by the BBT, using the parameters from WMAP, fits better to the data, including the error bars? [snip] Bye, Bjoern |
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References lost due to ISP problem.
"greywolf42" wrote in message ... George Dishman wrote in message ... snip higher stuff [You wrote: (attribution lost somewhere)] Light waves return a given fraction of their energy and momentum into the aether (or whatever is assumed by the specific tired light theory). Regardless of source. The "returning" is a local effect (at the point of fractional return). dE = - const E, at the point of inspection. The energy removed by tired light reduces over GPc distances so at short range is negligible. The energy per unit volume from a star then varies as the inverse square of the distance from the source Light energy from a star drops off below the inverse square distance law in the tired light model. so we should see a higher CMBR temperature looking along a line of sight that passes near to a star. No, because your starting assumption was wrong. My starting assumption was the same as you say above: "The 'returning' is a local effect (at the point of fractional return). dE = - const E, at the point of inspection." The E in that equation falls as the inverse square hence so does dE. I argued that we don't see this. I don't know of any reason that we should. The same applies at greater distances if we look along a line that passes close to, but not through a distant galaxy. Again this is not observed so conflicts with the suggestion that the source is illuminated in this way. Now I'm quite willing to believe I have simply not understood your model, but you need to explain this point if I am to understand. Explanation provided above. Your hand-wave (unquantified) argument was based on a bad assumption. I don't think so. It still seems to me that dE in the equation you posted will follow an inverse square from each (point) source of E. In other areas however, you have said that the aether is at a uniform temperature. I've said that we don't expect it to be heated in the local region of stars. It is roughly uniform. I'll respond separately on that basis, this is just a point of curiosity. George |
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First I'll draw together a few bits that I think
sum up most of the relevant parts of the discussion though it's quite possible I'll miss some. line length reduced in quoted material to minimise problems later "greywolf42" wrote in message ... George Dishman wrote in message ... snip In other areas however, you have said that the aether is at a uniform temperature. I've said that we don't expect it to be heated in the local region of stars. It is roughly uniform. snip .... There is no significant change in temperature with distance and time. "greywolf42" wrote: George Dishman wrote in message ... "greywolf42" wrote in message .. . snip For example, in my favorite theory (a Maxwellian/ LeSage theory), the CMBR is simply an EM hum from electrons bound to hydrogen. But that doesn't produce the spectrum we see, Sure it does. It's a thermal emission. .... lambda = (1.0E-30) (2.99e+8) / (1.602E-19) = 1.87 E-3 m Computing the equivalent blackbody temperature spectrum of this emission gives: T = .51 / 100 lambda = 2.73 deg K. "greywolf42" wrote in message ... snip ... Extinction due to grey dust is not contained in any tired light theory. Only in strawmen. Hence I frankly don't care to go out on another tangent. "greywolf42" wrote George Dishman wrote: snip If he can come up with one that explains the spectrum of the CMBR Electron vortex noise from the aether. A local effect due to electrons bound in hydrogen gas. and its dipole moment The motion of the solar system through the aether. as well as why the cosmological red-shift is exponential with distance Any tired light theory. (In this case, the slight imperfection in the aether.) "greywolf42" wrote in message ... George Dishman wrote in message ... snip Cloud emissions show different spectra which we can use to determine temperature while the CMBR is remarkably uniform. The local region of space (a few tens of parsecs) is expected to have an aether that is remarkably uniform in temperature. "greywolf42" wrote in message ... George Dishman wrote in message ... snip The extra factor to be taken into account in this case would be the electron density. Nope. Electron density wouldn't change anything. The temperature might be the same everywhere but the intensity radiated would be higher in regions with more electrons. Again, you are thinking cosmogenic. "greywolf42" wrote in message ... George Dishman wrote in message ... "greywolf42" wrote in message ... That's why I said I'd work with your numbers. Let's keep it simple. One does not need to have all the answers at the beginning..... OK, that will let me illustrate how I think Ned's test applies. I'll essentially throw a strawman at you and you can then correct the errors in my understanding of your model and we will see if that solves the problem. Just doing the best you can with your view of Ned's site will be fine. But use a *real* tired light theory. (i.e. Vigiers.) I have no desire to deal with yet another strawman. Ok, I think we have enough to try this with what you've said. The aim is partly show how Ned's test can be applied and also to give a starting point so that you can try to produce a self-consistent model that explains the spectrum of the CMBR. If you want to use Vigier or whatever, feel free but I don't expect you to say explanation A can produce the spectrum while explanation B can explain the dipole if A and B are mutually exclusive. As you said, we don't need to have all the answers at the beginning but we should be able to sort them out in the course of the discussion. So the strawman is this: -:- Postulates: The CMBR is produced by "Electron vortex noise from the aether, a local effect due to electrons bound in hydrogen gas." The electrons are producing a blackbody spectrum at an equivalent temperature of roughly 2.73K. The solar system is moving through this hydrogen and as a result there is a Doppler effect which produces the cosmic dipole moment. This "electron hum" is produced everywhere roughly uniformly as the electron density does not affect the emitted intensity. Each photon of this emitted radiation loses energy at a rate given by dE/E = dl/L due to a slight imperfection in the aether. The value of L is approximately 4.2GPc give or take a factor of 2. This is independent of frequency producing an exponential reduction of energy with distance. While the defect reduces the energy of individual photons, it does not absorb photons. There is no significant reduction of photon numbers due to grey dust or other possible causes of extinction. The energy lost is transferred to the aether and replaces the energy used locally to emit the CMBR photons, hence energy is locally conserved. -:- To analyse the above using Ned's test, we split the universe around the solar system into thin, concentric spherical shells or thickness dR at radius R. The surface area of each shell can be thought of as composed of many small cells of volume dV and the number of such cells is R^2*dR/dV. Ignoring tired light energy loss, the amount of radiation we receive from each cell is proportional to R^-2 (inverse square law) and proportional to dV hence the total rate of photons from each shell is independent of R. However, depending on the "cross section" of an electron, it may be only a fraction k of the amount that would be emitted by a solid (opaque) surface. This factor k is adjustable. The total radiation we receive is then the sum of the photons from all the shells, however each photon will be measured at a frequency which has been reduced from that at which it was transmitted by the tired light effect. http://www.astro.ucla.edu/~wright/tiredlit.gif Looking at Ned's graph, the local (z ~ 0) electron hum would be measured as the black line other than being scaled down by the factor k. However, to that we must add contributions from greater distances since there is no appreciable extinction. First think of a series of shells at z=0.1, z=0.2, etc.. Each would produce a curve similar to the black line with the same peak intensity but with the peak frequency moved to the left. The total would then be the sum of an infinite series of such curves. It should be clear that essentially the total observed curve becomes something like a straight line to the left (lower frequency) of the locally generated peak. Of course the series of discrete shells is an approximation as the source is continuous so to find the real prediction let dR tend to zero and integrate instead of summing. The overall intensity of the curve can be adjusted by changing k but the intensity will always be too high at frequencies below the peak for a blackbody. In fact I don't think you will get a peak at all. I've spent too much time putting this together and I don't want to spend more time doing the integration, I think I've said enough so you can if you wish. The point is that, with the stated strawman, the observed spectrum will not match a blackbody. So the question is can you change the strawman, or indeed discard it entirely and replace it with a real tired light theory, and show that you can then match the observed spectrum while still explaining the dipole? George |
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George Dishman wrote in message
... References lost due to ISP problem. "greywolf42" wrote in message ... George Dishman wrote in message ... snip higher stuff [You wrote: (attribution lost somewhere)] Light waves return a given fraction of their energy and momentum into the aether (or whatever is assumed by the specific tired light theory). Regardless of source. The "returning" is a local effect (at the point of fractional return). dE = - const E, at the point of inspection. The energy removed by tired light reduces over GPc distances so at short range is negligible. The energy per unit volume from a star then varies as the inverse square of the distance from the source Light energy from a star drops off below the inverse square distance law in the tired light model. so we should see a higher CMBR temperature looking along a line of sight that passes near to a star. No, because your starting assumption was wrong. My starting assumption was the same as you say above: "The 'returning' is a local effect (at the point of fractional return). dE = - const E, at the point of inspection." Sorry, I did not consider that your starting assumption, because of the large gap -- and because the next statement does not follow from the above. The E in that equation falls as the inverse square This is your incorrect assumption. The E in the above equation does not fall as the inverse square. The equation above is the pure linear form. The only degradation is due to the fractional removal from every photon (which continues in a straight line). Inverse square is the reduction in the number of photons per unit area, as a spherical source spreads over the surface of larger spherical shells. hence so does dE. I argued that we don't see this. I don't know of any reason that we should. The same applies at greater distances if we look along a line that passes close to, but not through a distant galaxy. Again this is not observed so conflicts with the suggestion that the source is illuminated in this way. Now I'm quite willing to believe I have simply not understood your model, but you need to explain this point if I am to understand. Explanation provided above. Your hand-wave (unquantified) argument was based on a bad assumption. I don't think so. It still seems to me that dE in the equation you posted will follow an inverse square from each (point) source of E. As demonstrated above, you are incorrect. A tired light model will always be (slightly) below a pure inverse square model. In other areas however, you have said that the aether is at a uniform temperature. I've said that we don't expect it to be heated in the local region of stars. It is roughly uniform. I'll respond separately on that basis, this is just a point of curiosity. Curiosity is good. Though it is rough on cats. ![]() -- greywolf42 ubi dubium ibi libertas {remove planet for return e-mail} |
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