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#210 | |
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May 2004
New York City
10000100010112 Posts |
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existed, and that its "explosion" or "expansion" initiated the generation of our current Universe, some large finite time ago, how do you resolve the issue that there is no reason to consider that event the "beginning" of anything? And if you accept that the initiation of that event was preceded by any amount of time, that in fact time goes back forever, of what special significance is the bang (if it really occurred)? I stand by my monograph (draft 2 is in the works) with rejection of the BBT as an unnecessary hypothesis used to scientifically cloak a Creationism viewpoint. The Universe has always existed. There are no singularities. |
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#211 | |
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Bamboozled!
"πΊππ·π·π"
May 2003
Down not across
22·5·72·11 Posts |
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If you wish to dive into the literature, where some suggestive observational support has been presented, the phrase "Conformal Cyclic Cosmology" will prove helpful. Paul |
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#212 |
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May 2004
New York City
5·7·112 Posts |
Yes indeed an infinite repetition of small singularity through expansion to
infinite dispersion, regressed backwards through time and unfolding again through the future, does satisfy the infinity of time in the Universe, and automatically removes the word "the" from "the Big Bang", since there were infinitely many in the past and will be again. But there can not ever be any observable evidence to support this concept, all evidence of previous Bangs would be wiped out by necessity and the definition of a singularity. I agree that there is a cyclic galactic generation process within the Universe, but not for the Universe as a whole. |
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#213 | |
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Bamboozled!
"πΊππ·π·π"
May 2003
Down not across
101010000111002 Posts |
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Whether evidence can or can not be observable is something which can be tested by observation. CCC makes a clear prediction of effects which can in principle be observed. Paul |
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#214 | ||
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"Richard B. Woods"
Aug 2002
Wisconsin USA
22·3·641 Posts |
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#215 | |||
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May 2004
New York City
10000100010112 Posts |
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the fourth spatial dimension (skin) at every frequency, but moreso at the lower wavelengths / higher frequencies because the pinholes in the skin act "like" a diffraction grating and admit more EMR if the wavelength is smaller, according to some distribution function, calculable from the degree of shift. So the process both dims the received light and redshifts the whole spectrum. No space expansion or spreading out of photons is necessary. If that explanation is insufficient, I'd be glad to hear the reason. My monograph is, after all, a work in progress. Last fiddled with by davar55 on 2011-05-24 at 13:47 Reason: fixde typo |
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#216 | |
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"Richard B. Woods"
Aug 2002
Wisconsin USA
22·3·641 Posts |
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Example, Part A Suppose there's an absorption line at 6550 angstroms (from a source stationary with respect to the observer) and this results in the following reading from a digital spectroscope: Code:
Wavelength Intensity of light at that wavelength 6545 0.99 6546 0.99 6547 0.99 6548 0.99 6549 0.97 6550 0.05 6551 0.97 6552 0.99 6553 0.99 6554 0.99 6555 0.99 Code:
Wavelength Intensity of light at that wavelength, in some unit 6545 0.99 6546 0.99 6547 0.99 6548 0.99 6549 0.99 6550 0.99 6551 0.97 6552 0.05 6553 0.97 6554 0.99 6555 0.99 (Now, that is just the first part. Once you explain that, I'll present the next part.) Last fiddled with by cheesehead on 2011-05-24 at 18:37 |
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#217 | |
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May 2004
New York City
423510 Posts |
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Shouldn't the 6550 spectral line be at HIGHEST intensity, not lowest, e.g. 0.99 with the nearbys lower (like 6552 at 0.97 but not nearly low like 0.05)? Then a FURTHER star might see some of the 6550 diminished to 0.97, and 6552 because its a higher wavelength diminished by a smaller amount to 0.96, but still a local peak? I'm not sure this is convincing, but consider my first point, that spectral lines represent peaks. |
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#218 | |
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Oct 2007
Manchester, UK
22·3·113 Posts |
If stars or galaxies were perfect blackbody emitters, then they would have perfect black body spectra dictated only by their temperature. But they don't, because they aren't. Instead you get dips in the spectrum dictated by the absorption spectra of the various elements in the emitter, which for stars is overwhelmingly hydrogen, then helium, then increasingly trace amounts of oxygen, carbon, nitrogen and so on.
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#219 | ||
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"Richard B. Woods"
Aug 2002
Wisconsin USA
22·3·641 Posts |
A) My example didn't specify a star or galaxy -- just "source".
I intend that the (idealized) source has a continuous blackbody emission spectrum overlaid by a discrete line from absorption by a cooler gas layer around the central continuous emitter. B) My example doesn't deny the existence of spectrum outside of the 6545-6555 range. I'm just asking you for your theory's explanation of example observations in that range. Quote:
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B) Your "first point" where? I don't see where your "first point, that spectral lines represent peaks" is. It's certainly not first in cosmo1.txt, In fact, cosmo1.txt doesn't contain either of the words "spectral" or "peak", and the only occurrences of "line" are in the phrase "traveling in a straight line". Last fiddled with by cheesehead on 2011-05-25 at 01:12 Reason: correc- and addi-tions |
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#220 | |
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May 2004
New York City
5·7·112 Posts |
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was accomplished in finite time. Or does his process allow actual infinities of time and space? |
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