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![]() "Henri Wilson" HW@.... wrote in message news ![]() On Thu, 30 Aug 2007 17:17:24 +0100, "George Dishman" wrote: "Henri Wilson" HW@.... wrote in message . .. The temperature of all layers should increase as the star contracts under gravity. Sure, both factors operate. I think you haven't previously looked at a typical temperature curve. I have....and it is willusory anyway... Nope, other than time of arrival, the temperature is a ratio of bands so isn't affected. The 'ratio of bands' is very sensitive to the type of radiator. Any variation from black body could have a profound effect. Indeed and care must be taken for that reason especially with local factors like absorption by water and oxygen in the K band. These effects are well known though, nobody ignores them. ....but everybody seems to ignore the most critical factor..that of variable light speed.... People take the frequency dependence of the refractive index into account where it has an effect, e.g. in pulsar dispersion. The cause doesn't matter, the shift is less than 0.01% or 0.22nm for K band when the filter is 400nm wide - completely negligible. You cannot assume a consant emissivity for the changing surface layer either. The emissivity is 100% at the bottom of the layer Henry, Kirchoff's law requires that. Not if its temperature is continually changing. Yes Henry, Kirchoff's law requires it. Nor can you have photons with negative lengths... That's your 'wave equation' of course.... No that's YOUR 'wave model', you have no wave equation. Photons are particles. Right, but you don't have an equation for that either. No you aren't. You didn't even consider the main factor, the temperature gradient in the water and its affect on viscosity.... We know the ball's volume will decrease nonlinearly and we can assume it remains in temperature equilibrium with the water. The sea's temperature changes only slightly with depth after the first few tens of metres, and the effect on the ball will be minimal. Viscosity has no effect at all on the volume of the ball. I know that George. Thank goodness. I'm talking about the rate of fall, ... No, you were talking about the ball being compressed by pressure as an analogy for a photon being squeezed by the differential velocity due to acceleration at the time of emission, or some such rubbish, you never mentioned rate of fall. I don't see how Kirchoff's law really comes into this. Sure the emissivity of the surface is likely to change with both temperature and density but the law will still hold. Since the gas is a black body radiator, it must also be a perfect absorber. As the density rises, it becomes completely opaque which is why you cannot see through to a second layer. they are big assumptions... Nope, they are results confirmed by lab tests. The models at first could not get the 10 day period right for the in-phase 'bump' no matter how people tried to adjust them. The opacity of He++ was rechecked and found to be wrong and that solved the problem. The essence of a good model is that is _cannot_ be made to match unless the parameters are valid, unlike your excellent match to the theme from Close Encounters with your "Keplerian Orbits Only" program. ......so you believe that cepheid curves are Keplarian out of pure coincidence? No, I believe you have added so many adjustable parameters in your program that you can fit any curve, Keplerian or not. George, the well known cepheid curve is Keplerian...whether you like it or not... Nope, but your program can produce almost any curve, Keplerian or not so that's not a problem for you. George |
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