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![]() "greywolf42" wrote in message ... George Dishman wrote in message ... much snipped again to get to the physics, some parts moved 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. The "per Hz" does not compensate for this effect. Ned's curve appears to show a shift *without* energy removal. ... part from later in your replay brought forward Tired light effectively compresses the power emitted into a narrower band. Umm, no. Tired light does not compress power bands. This may simply be a sloppy usage on your part. The relative energy-frequency curve merely shifts. It does not compress the band, unless you arbitrarily have set a minimum intensity as defining the edges of the "band." Think of the graph as a histogram with bins 1Hz wide, that's what sets the edges. The photons that go into a bin from f to f+1 on the red curve come from frequencies in the range 1.1*f to 1.1*(f+1) on the blue curve. That's 10% more photons than are in the corresponding bin on the blue curve which is from (1.1*f) to (1.1*f)+1. Of course each photon carries 10% less energy so the two factors cancel and the intensity is the same. Take a more extree example, consider a source received with z=2. Suppose you measure the intensity at 1MHz. That is a measure of the power in the band from 1,000,000Hz to 1,000,001Hz. However when the photons were emitted they had frequencies from 2,000,000Hz to 2,000,002Hz When put into the histogram though, that range would be split into two bins, the first from 2,000,000Hz to 2,000,001Hz and the other from 2,000,001Hz to 2,000,002Hz. There are therefore twice as many photons in the bin for the received intensity as in each of the bins for the emitted intensity, but since each received photon has half the energy when it was transmitted, the total power in each 1Hz band is the same. Do you follow yet, it's not my best explanation. ... Note that the "resultant" (red) curve has the perfect shape to match the observations -- if you merely divide the intensity values by Ned's arbitrary factor of 1.331. That's right, so if the source was say rocks at that temperature and the rocks only covered 75.13% of the sky then the intensity would be just right. Similarly if the rocks were at 3.27K and z=0.2 then they would need to cover exactly 57.87% of the sky to match observation. I think that might be one of the possible coincidences that Ned mentions, that to explain the observation, the amount of sky covered would have to be exactly (1+z)^-3 Let's take a quick look at Ned's support for his curves: "Assume that the CMB starts out as a T = (1+z)*To = 2.998 K blackbody, which is the blue curve. Because the photons only lose energy but do not decrease their density, the resulting red curve is not a blackbody at To = 2.725, but is instead (1+z)3 = 1.331 times a blackbody." Now where do *you* get Ned's "original" intensity for the blue curve? I cannot determine this from your interpretation of Ned's test. For the intensity would be based on the density of your source gas shell. I haven't checked the values but I assume it is simply Planck's Law, in other words it covers the whole sky. snip ... Tired light theories do not need nonlocal sources. In this case, "nonlocal" means "outside of the receiving apparatus." 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. I'm *not* addressing what designers typically consider "thermal noise" of the receiver. That is merely the noise due to the temperature of the matter -- which varies with matter temperature. What I am referring to is the aether electron "hum" that arises from the interaction of the electron (standing wave) with the aether corpuscles. Not one CMBR device -- to my knowledge -- has ever attempted an isolation test. That is, a test to determine whether the signal was actually produced "within" the antenna -- or whether it had an external source. For example, I know for a fact that Penzias and Wilson did not do this test. They *did* cut out the antenna connection. But they did not put their antenna in an isolation chamber. I'd be happy to be corrected, if you know of anyone who has done this. (And this has been discussed on the newsgroups for at least a decade.) Well I can't imagine they would launch any craft without testing the equipment and you can't do that except in a screened room. However, you would have to contact the team that built the equipment to get confirmation, it's the sort of thing everyone does without comment, just normal engineering, so it is unlikely you will find anything published about it. Perhaps it is simpler just to point out that since COBE and WMAP produce the same map of the sky, the data cannot be an artefact of the detector. Obviously the resolution of WMAP is far better but just calculate the correlation of the two. I thought you said the CMBR was emitted by electrons being excited by the aether, Yes. I have attempted to clarify the situation for you. *ALL* electrons are effected by the aether. As you said, the dipole indicates that the source of the radiation is moving past the detector. If this is "electron hum" from electrons bound in hydrogen as you said, then that hydrogen must be flowing past the craft at about 400km/s and the hydrogen is moving in the same direction regardless of which way the craft is pointed. Including the antenna of the Penzias and Wilson device, and all other such devices. No experimental system that I am aware of, has ever tested to eliminate this possibility. P&Z never made this test. After P&Z, everyone simply assumed it was "cosmic" in origin (i.e. outside the mechanism) -- and never made this test. How do you think they would calibrate an instrument that was picking up every microwave oven and mobile phone for miles around? All such testing and calibration has to be done in an electrically quiet environment and that means a screened room. However, what would be the point? If this noise is generated by hydrogen in matter anyway, it would still fill any EMC chanber as well. ... 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. That is *your* description. Unfortuantely, Ned doesn't provide any such description. What he provides is just this: "The expanding balloon analogy for cosmological models can be used to show this. ... Note that the galaxies (yellow blobs) do not grow, but the distance between galaxies grows, and that the photons move and shift from blue to red as the Universe expands, and the photon density goes down. But in the tired light model, illustrated below, the density does not go down. Assume that the CMB starts out as a T = (1+z)*To = 2.998 K blackbody...." AFAICT, Ned *IS* specifically addressing the expanding balloon analogy of the BB. And Ned *IS* therefore specifically addressing the fact that the "temperature of space" is cooling. Your approach would need no reliance upon the BB balloon analogy at all. snip *NED's* model is the BB balloon universe. The temperature varies with time. *YOUR* model does not. The top two circles show the balloon analogy for the big bang. The balloon on the right is bigger and the effect of expansion is both to redden the light (the blue squiggly lines become red ones) but also to increase the volume of space as the cube of the expansion. The fact that the same number of photons are skulling around in a bigger volume si what reduces the density. In contrast, the next pair of circles represents a steady- state model so the two circles are the same size - no expansion. Tired light still reddens the light but the density of squiggly lines remains the same. That's why there's a difference of (1+z)^3 between the two models. Note that in this pair, there is _no_ expansion of the balloon, that's the whole point. Only by keeping the size the same can he illustrate that the volume doesn't change hence the photon density doesn't change, only the individual energies. George |
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