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Re: Hubble deep field question
| John Polasek | 28 Jan 2009 15:51 |
>Dear John Polasek: > [quoted text clipped - 19 lines] > >But you did invoke straight classical Doppler shift, which, I think you will agree, is merely the most plausible *explanation* for a universally acknowledged phenomenon, redshift, and which involves mere kinematics.
>with the inherent >energies required to blast masses away from us at significant >percentages of the speed of light. You seem to have accepted the responsibility of providing an explanation for Doppler redshift, but I resent your making me a party to this hypothetical detonation.
In any case, this dynamite thing is just an obfuscatory distraction, which in no way undermines my assertion that z/1+z is the proper distance modulus, not z.
You stated that recession velocity at z =1 is c, and tolerated a reported measurement of z = 6 making v = 6c, without considering how you could see the redshift. Of course with D = z/1+z you get v = c*6/7 and we are back in real physics.
>> My statement treats of a line joining the >> observer and his star- there's no explosion. [quoted text clipped - 4 lines] >> I repeat, it is a serious error with serious >> consequences The inherent error lies in failing to recognize that while the Doppler effect has a transparent explanation as a frequency phenomenon, it is *measured* as a wavelength phenomenon and then persisting to employ wavelength algebra through thick and thin despite the glaring incongruities.
>You are right. So why don't you face those consequences? You better modify all those z*c expressions to zc/1+z.
>David A. Smith John Polasek
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| dlzc | 27 Jan 2009 14:45 |
Dear John Polasek:
> >> On Thu, 22 Jan 2009 17:00:01 -0700, "N:dlzcD:aol T:com \(dlzc\)" > [quoted text clipped - 15 lines] > > I did not discuss 'center'. But you did invoke straight classical Doppler shift, with the inherent energies required to blast masses away from us at significant percentages of the speed of light.
> My statement treats of a line joining the > observer and his star- there's no explosion. Sure, if you completely ignore what your "model" requires.
...
> I repeat, it is a serious error with serious > consequences You are right. So why don't you face those consequences?
David A. Smith
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| John Polasek | 26 Jan 2009 22:14 |
>Dear John Polasek: > [quoted text clipped - 16 lines] > >David A. Smith I did not discuss 'center'. My statement treats of a line joining the observer and his star- there's no explosion.
I derived the velocity for you as a function of z, but you neglected to examine it.
No center you say, OK, but then space has no substance either, that could stretch by 1+z, ostensibly to fend off superluminal problems. But these problems stem from erroneous use of the illegal expression cz leading to 2c, 3c, which are not impossible, just that there's nothing to see past 1c and we need to see redshift. The red shift is from Doppler alone, but a whole legend has developed from this 1+z stretch fixation. The paper below argues for a replacement of z with z/1+z but from purely mathematical consideration of algebraic poles and the like. http://arxiv.org/abs/ 0710.1887. This notion is correct as I have shown in the prior note.
I repeat, it is a serious error with serious consequences
John Polasek
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| dlzc | 26 Jan 2009 18:33 |
Dear John Polasek:
> On Thu, 22 Jan 2009 17:00:01 -0700, "N:dlzcD:aol T:com \(dlzc\)" > [quoted text clipped - 8 lines] > I beg to differ. This is a common and grievous > error, if we attribute redshift to straight Doppler. The Universe has no unique center, therefore the expansion is not from an explosion in space. So there is no theoretical support to your "manipulations".
David A. Smith
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| John Polasek | 24 Jan 2009 04:51 |
On Thu, 22 Jan 2009 17:00:01 -0700, "N:dlzc D:aol T:com \(dlzc\)" <dlzc1@cox.net> wrote:
>Dear Craig Franck: > >"Craig Franck" <craig.franck@verizon.net> wrote in message >snip > >No. A Z of 1 is "receeding" at c. I beg to differ. This is a common and grievous error, if we attribute redshift to straight Doppler. The laboratory measurement is L'/L = 1 + z Letting v/c = b (for beta), doppler causes the frequency reduction f'/f = 1 - b from which the wavelength is given by the inverse L'/L = 1/1-b = 1 + b + b^2 + b^3 which is not 1 + z z is not v/c. A little algebra shows that recession velocity is given by c*z/1+z, so for z = 1, the recession is c/2. I think this has been lost sight of in the current fiction that space stretches wavelengths by 1+z, a concept which panders to Einsteins space-time. I see the graphs that routinely present v/c>1 with velocities equal to 2 and 3c. It isn't true, and this is the reason, which should come as a great relief, since viewing >c is impossible.
>http://www.astro.ucla.edu/~wright/cosmo_01.htm >... the text below the little sketch with the text "You're >receding" > >David A. Smith John Polasek
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| N:dlzc D:aol T:com (dlzc) | 23 Jan 2009 00:00 |
Dear Craig Franck:
> I'm reading "Chasing Hubble's Shadows" by Jeff > Kanipe, and he states on page 140 that "blobjects" > at redshift 6 that were 13,000 light years across > would appear 0.2 seconds of arc in size. But that's > assuming the light left when the object was 12.7 > billion light years away. No,, that assumes the objects look to be 12.7 Gly away "now".
> I had thought that the objects would have been > much closer when the light first left and it took > 12.7 billion years to reach us because of cosmic > expansion, which would not have made the > objects look smaller. ... and hence further away, and with the correct intensity.
> At redshift 6 they would be traveling at about > 0.9c, No. A Z of 1 is "receeding" at c.
http://www.astro.ucla.edu/~wright/cosmo_01.htm ... the text below the little sketch with the text "You're receding"
> but how would you figure out how far away they > were when the light first left from that? I thought it > would be 1/6 * 12.7bly, but that's assuming the > author is wrong, which may not be warranted. I think you are trying to get to a number that has little meaning.
David A. Smith
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| Craig Franck | 22 Jan 2009 22:55 |
I'm reading "Chasing Hubble's Shadows" by Jeff Kanipe, and he states on page 140 that "blobjects" at redshift 6 that were 13,000 light years across would appear 0.2 seconds of arc in size. But that's assuming the light left when the object was 12.7 billion light years away.
I had thought that the objects would have been much closer when the light first left and it took 12.7 billion years to reach us because of cosmic expansion, which would not have made the objects look smaller.
At redshift 6 they would be traveling at about 0.9c, but how would you figure out how far away they were when the light first left from that? I thought it would be 1/6 * 12.7bly, but that's assuming the author is wrong, which may not be warranted.
 Signature Craig Franck craig.franck@verizon.net Cortland, NY
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