|
|
|
Thread Tools | Display Modes |
#11
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
Dear John C. Polasek:
On Aug 15, 6:50 pm, John C. Polasek wrote: On Wed, 15 Aug 2007 09:09:52 wrote: Dear John C. Polasek: On Aug 14, 6:00 pm, John C. Polasek wrote: ... I think the solution is a lot easier than jiggling with G. Isn't redshift the only way to measure such distances? They find that the observed intensity is less than expected from red-shift distance. No, redshift is not the only way. If there are type Ia supernovae located in the "structure", there is the duration of the decay from peak to some percentage of peak. There is intensity of the source (1/r^2, regardless of source... *assuming* something about the source). All these methods agree to within the margin of error in the paper I saw. I didn't mean it's the only way; I meant it conflcts with the intensity readings. The only paper that I am aware of, *all* the disparate measurements agree to within their margin of error. The disparity between redshift and intensity Do you have a citation? Is intensity higher or lower than redshift would indicate? is what's causing all the expansion talk. Expansion is what redshift (and stretching of duration, and decrease in intensity) is all about. The "disparity" serves to describe something other than expansion. There are a pretty good number of factors that can produce this disparity, although anomalously more intensity with distance might be a bit of a challenge. There's no agreement except as to disagreement. And so I'm asking the modality of the red shift / distance calculation, is it doppler, is it scale factor, is it the relativistic doppler? http://www.astro.ucla.edu/~wright/cosmo_01.htm ... so you get from 1+z to distance via a linear transformation ("scale factor"). Doppler really doesn't give you distance, just change in distance. And you can't integrate over time, because we don't know the time without *assuming* what we set out to measure. The discrepancy might be corrected with proper algebra, instead of dark energy. Get rid of Dark Matter, and there is almost no need for Dark Energy. MOND almost works, and TeVaS does work (as far as I know) at getting rid of Dark Matter. David A. Smith |
#12
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
On Thu, 16 Aug 2007 07:44:41 -0700, dlzc wrote:
Dear John C. Polasek: On Aug 15, 6:50 pm, John C. Polasek wrote: On Wed, 15 Aug 2007 09:09:52 wrote: Dear John C. Polasek: On Aug 14, 6:00 pm, John C. Polasek wrote: ... I think the solution is a lot easier than jiggling with G. Isn't redshift the only way to measure such distances? They find that the observed intensity is less than expected from red-shift distance. No, redshift is not the only way. If there are type Ia supernovae located in the "structure", there is the duration of the decay from peak to some percentage of peak. There is intensity of the source (1/r^2, regardless of source... *assuming* something about the source). All these methods agree to within the margin of error in the paper I saw. I didn't mean it's the only way; I meant it conflcts with the intensity readings. The only paper that I am aware of, *all* the disparate measurements agree to within their margin of error. The disparity between redshift and intensity Do you have a citation? Is intensity higher or lower than redshift would indicate? is what's causing all the expansion talk. Expansion is what redshift (and stretching of duration, and decrease in intensity) is all about. The "disparity" serves to describe something other than expansion. There are a pretty good number of factors that can produce this disparity, although anomalously more intensity with distance might be a bit of a challenge. There's no agreement except as to disagreement. And so I'm asking the modality of the red shift / distance calculation, is it doppler, is it scale factor, is it the relativistic doppler? http://www.astro.ucla.edu/~wright/cosmo_01.htm .. so you get from 1+z to distance via a linear transformation ("scale factor"). Doppler really doesn't give you distance, just change in distance. It should give recession velocity, from which a proper H0 would give distance. And you can't integrate over time, because we don't know the time without *assuming* what we set out to measure. The discrepancy might be corrected with proper algebra, instead of dark energy. Get rid of Dark Matter, and there is almost no need for Dark Energy. MOND almost works, and TeVaS does work (as far as I know) at getting rid of Dark Matter. David A. Smith Excuse my error: what I meant was acceleration, not expansion. Acceleration of expansion rate is the current big phenomenon being investigated, in which it is universally presented that the observed intensity of SN1A's is lower than might be expected by square law 1/D^2. No question, you can measure redshift. From it there are several ways of deducing distance. But nowhere do I see it displayed, what equation is being used. From astro.ucla (above) you imply a/a0 = 1+z from which 1/D^2 would be proportional to 1/(1+z)^2 but the observed intensity is markedly lower. Time dilation applied to the decay curve is some part of the analysis, but that calculation implies recession velocity, not a/a0. The papers I have read are quite abstruse, trying to get a handle on the impact of "quintessence", I believe. It seems there's plenty of places to scrutinize the transformation from redshift to distance or time dilation to distance, enough room for simple error to explain away acceleration. John Polasek |
#13
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
DEar John C. Polasek:
On Aug 16, 9:20 am, John C. Polasek wrote: On Thu, 16 Aug 2007 07:44:41 wrote: .... The disparity between redshift and intensity Do you have a citation? Is intensity higher or lower than redshift would indicate? .... http://www.astro.ucla.edu/~wright/cosmo_01.htm .. so you get from 1+z to distance via a linear transformation ("scale factor"). Doppler really doesn't give you distance, just change in distance. It should give recession velocity, from which a proper H0 would give distance. As you are aware, the value of H0 is applied directly to (1+z). .... The discrepancy might be corrected with proper algebra, instead of dark energy. Get rid of Dark Matter, and there is almost no need for Dark Energy. MOND almost works, and TeVaS does work (as far as I know) at getting rid of Dark Matter. Excuse my error: what I meant was acceleration, not expansion. Acceleration of expansion rate is the current big phenomenon being investigated, in which it is universally presented that the observed intensity of SN1A's is lower than might be expected by square law 1/D^2. Still, do you have a citation? No question, you can measure redshift. From it there are several ways of deducing distance. But nowhere do I see it displayed, what equation is being used. I believe it is straightforward, comparing intensity at characteristic times in the "decay curve", to more local "members of the SNIa community". I will have to review the pdf I have at home tonight, and I will reply to your message with a link on arxiv.org. From astro.ucla (above) you imply a/a0 = 1+z from which 1/D^2 would be proportional to 1/(1+z)^2 but the observed intensity is markedly lower. I don't find that in the paper, which is why I keep asking for a citation. Time dilation applied to the decay curve is some part of the analysis, but that calculation implies recession velocity, not a/a0. The papers I have read are quite abstruse, trying to get a handle on the impact of "quintessence", I believe. It seems there's plenty of places to scrutinize the transformation from redshift to distance or time dilation to distance, enough room for simple error to explain away acceleration. Much easier for me to believe that the Universe had more "free dust" in earlier ages, which would give lower intensities now. After all, we discuss how all these stars are forming, and planets are forming, and supernovae are more prevalent in earlier times... And even easier for me to believe that expansion (even without acceleration) is creating places that light could not possibly have been directed towards at the time of emission. Granted, this is an "infinitessimal, interstitial" creation... but we are not located entirely at the "spherical D surface" that the light was originally aimed at, but would have been apparently diced into little bits, and a good percentage of us was left out when reassembled to form the original target. To me it makes *sense* that intensity would be lower. David A. Smith |
#14
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
On Jul 30, 6:46?pm, wrote:
The Accelerating Universe and Decreasing Cosmic Gravity. By Louis Nielsen, Denmark http://www.rostra.dk/louis The discovery of the accelerating Universe could be an indication of a cosmic decreasing gravity. Observations of supernovae, belonging to distant galaxies, show that they are situated at distances that are greater than what would be expected according to current cosmological models. This must mean that the galaxies in question have moved faster than expected. The analysis of the observations shows that the rate of expansion of the Universe appears to vary with position. More distant objects are receding from us faster than nearby ones. That is, the expansion of the Universe was faster at earlier times than it is right now. To save the traditional cosmological models the scientists now try to introduce different solutions, supported by new and old effects, such as 'dark energy', 'dark-matter' and the re-introduction of the 'cosmological constant' in Einstein's general field equations, etc. Decrease of the Cosmic Gravity. But maybe the accelerated expansion of the Universe is an indication of a cosmic decrease of Newton's gravitational 'constant'. In my considerations about "Quantum Cosmology with Decreasing Gravity" I assume that Newton's gravitational 'constant' G is a decreasing quantity. (Read more in my treatise). The decrease of G with cosmic time is (in the continuous approximation) given by the equation: (1) (1/G)*(dG/dT) = - (1/3)*(1/T) (dG/dT is the time derivative) In equation (1) T is the actual age of the Universe. We note that G does not decrease linearly with the age of the Universe. The relative decrease of G had been faster when the Universe was younger. When the Universe came into being, during the first cosmic quantum time intervals, G decreased extremely fast, corresponding to what in the standard cosmological theory is called an 'inflation phase'. In our epoch G decreases very slowly, so slow that it has not hitherto been possible to measure directly. If we could measure the relative decrease of G with very high precision then the age of the Universe can be calculated from equation (1). Due to a decrease of the cosmic gravitational forces, the distance between two gravitating mass systems - for example two galaxies will increase as the Universe ages. As the relative decrease of Newton's gravitational 'constant' is not a linearly function of time, this is also not the case for the increase in distance between two gravitational attracting systems. We can assume that the variable Hubble parameter H has connection to the decreasing gravitational 'constant' G according to the relation: (2) H = - (1/G)*(dG/dT) = (1/3)* (1/T) The radial velocity v of an object is then given by the modified Hubble-relation: (3) v = H*D = - (dG/dT)*(1/G)*D = (1/(3*T))*D In equation (3) D is the distance to the object. According to equation (3) v depends on both the distance D to the object and the actual age T of the Universe when the light was emitted.From equation (3) we see that when T was smaller then v was higher. Therefore objects in the younger Universe had moved a greater distance If gravitylike everything else is quantized then what happens when you get to a point where there may/maynot be a graviton than calculated from the ordinary Hubble-relation. As our knowledge of the physical objects in the Universe is mainly obtained by analysis of the light emitted by the objects, it is also necessary to take into account the gravitational conditions when the light was emitted. For instance the gravitational shift of wavelength depends on the strength of the gravitational field in the position from which the light is emitted. Also other physical effects depend on the actual value of G. Best regards Louis Nielsen Denmark |
#15
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
On Thu, 16 Aug 2007 12:40:41 -0700, dlzc wrote:
DEar John C. Polasek: On Aug 16, 9:20 am, John C. Polasek wrote: On Thu, 16 Aug 2007 07:44:41 wrote: ... The disparity between redshift and intensity Do you have a citation? Is intensity higher or lower than redshift would indicate? ... http://www.astro.ucla.edu/~wright/cosmo_01.htm .. so you get from 1+z to distance via a linear transformation ("scale factor"). Doppler really doesn't give you distance, just change in distance. It should give recession velocity, from which a proper H0 would give distance. As you are aware, the value of H0 is applied directly to (1+z). ... The discrepancy might be corrected with proper algebra, instead of dark energy. Get rid of Dark Matter, and there is almost no need for Dark Energy. MOND almost works, and TeVaS does work (as far as I know) at getting rid of Dark Matter. Excuse my error: what I meant was acceleration, not expansion. Acceleration of expansion rate is the current big phenomenon being investigated, in which it is universally presented that the observed intensity of SN1A's is lower than might be expected by square law 1/D^2. Still, do you have a citation? No question, you can measure redshift. From it there are several ways of deducing distance. But nowhere do I see it displayed, what equation is being used. I believe it is straightforward, comparing intensity at characteristic times in the "decay curve", to more local "members of the SNIa community". I will have to review the pdf I have at home tonight, and I will reply to your message with a link on arxiv.org. From astro.ucla (above) you imply a/a0 = 1+z from which 1/D^2 would be proportional to 1/(1+z)^2 but the observed intensity is markedly lower. I don't find that in the paper, which is why I keep asking for a citation. One paper is http://www.pnas.org/cgi/reprint/101/1/8.pdf which is easy to read, whose title is Hubble's diagram and cosmic expansion. There are others. Fig. 6 shows the magnitude deviation d(m - M) for z's to 1 for several percentages of dark energy. Even better is http://www.astro.ucla.edu - Supernova Cosmology (which has Ned Wright's imprimatur it turns out). Time dilation applied to the decay curve is some part of the analysis, but that calculation implies recession velocity, not a/a0. The papers I have read are quite abstruse, trying to get a handle on the impact of "quintessence", I believe. It seems there's plenty of places to scrutinize the transformation from redshift to distance or time dilation to distance, enough room for simple error to explain away acceleration. Much easier for me to believe that the Universe had more "free dust" in earlier ages, which would give lower intensities now. After all, we discuss how all these stars are forming, and planets are forming, and supernovae are more prevalent in earlier times... And even easier for me to believe that expansion (even without acceleration) is creating places that light could not possibly have been directed towards at the time of emission. Granted, this is an "infinitessimal, interstitial" creation... but we are not located entirely at the "spherical D surface" that the light was originally aimed at, but would have been apparently diced into little bits, and a good percentage of us was left out when reassembled to form the original target. To me it makes *sense* that intensity would be lower. We could make better progress if relativity had viable model, but it proposes a universe that is homogeneous, isotropic and without a center, (leaving us essentially without a handle) so even the cause of expansion is left to hypothesis, not excepting the unblushing use of dark energy and quintessence and matter/radiation percentages. Still can't find the z/distance transform. (It may come as a surprise that I have my own theory on the structure of the universe). David A. Smith John Polasek |
#16
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
Dear John C. Polasek:
On Aug 16, 8:32 pm, John C. Polasek wrote: On Thu, 16 Aug 2007 12:40:41 wrote: .... From astro.ucla (above) you imply a/a0 = 1+z from which 1/D^2 would be proportional to 1/(1+z)^2 but the observed intensity is markedly lower. I don't find that in the paper, which is why I keep asking for a citation. One paper is http://www.pnas.org/cgi/reprint/101/1/8.pdf which is easy to read, whose title is Hubble's diagram and cosmic expansion. There are others. Fig. 6 shows the magnitude deviation d(m - M) for z's to 1 for several percentages of dark energy. Thanks. Even better is http://www.astro.ucla.edu- Supernova Cosmology (which has Ned Wright's imprimatur it turns out). OK. I apologize, I forgot to look up that paper, which I believe has the intensity formula in it. I will do this tonight. I don't think it is more complex than: I_1 / I_2 = (R_2 / R_1)^2 ... using a "standard candle" for I_1 and R_1, measuring I_2, and solving for R_2. Some "standard candles": http://csep10.phys.utk.edu/astr162/l...y/cosmicd.html (which you proabably already know) Time dilation applied to the decay curve is some part of the analysis, but that calculation implies recession velocity, not a/a0. The papers I have read are quite abstruse, trying to get a handle on the impact of "quintessence", I believe. It seems there's plenty of places to scrutinize the transformation from redshift to distance or time dilation to distance, enough room for simple error to explain away acceleration. Much easier for me to believe that the Universe had more "free dust" in earlier ages, which would give lower intensities now. After all, we discuss how all these stars are forming, and planets are forming, and supernovae are more prevalent in earlier times... And even easier for me to believe that expansion (even without acceleration) is creating places that light could not possibly have been directed towards at the time of emission. Granted, this is an "infinitessimal, interstitial" creation... but we are not located entirely at the "spherical D surface" that the light was originally aimed at, but would have been apparently diced into little bits, and a good percentage of us was left out when reassembled to form the original target. To me it makes *sense* that intensity would be lower. We could make better progress if relativity had viable model, but it proposes a universe that is homogeneous, isotropic and without a center, Which simply means we are not in a special place, that we can guess what other places would see *now*... in general. Otherwise we'd have to make up special rules for places we cannot see, and we have no basis upon which to do that. "There be Langoliers..." (leaving us essentially without a handle) so even the cause of expansion is left to hypothesis, Actually theory... the second law of thermodynamics (SLT). Additional space equates to additional states, something that SLT does not allow reduction in. not excepting the unblushing use of dark energy I agree here. How is "energy" necessary if gravitation is not a "force"? But like the "Big Bang" and "E=mc^2" for even motion energies, things tend to stick. and quintessence and matter/radiation percentages. Still can't find the z/distance transform. I promise I'll get the link tonight. (It may come as a surprise that I have my own theory on the structure of the universe). Everyone does, which is why research exists. We can't believe it is that "hard" or that "odd" or even that "marvelous". David A. Smith |
#17
|
|||
|
|||
The Accelerating Universe and Decreasing Cosmic Gravity
Dear John C. Polasek:
On Aug 16, 8:32 pm, John C. Polasek wrote: On Thu, 16 Aug 2007 12:40:41 wrote: .... and quintessence and matter/radiation percentages. Still can't find the z/distance transform. I promise I'll get the link tonight. http://arxiv.org/abs/astro-ph/0104382 David A. Smith |
|
Thread Tools | |
Display Modes | |
|
|
Similar Threads | ||||
Thread | Thread Starter | Forum | Replies | Last Post |
Expanding Universe - Accelerating | TeaTime | UK Astronomy | 0 | November 23rd 06 01:46 AM |
Accelerating Motion and Spin = Gravity | G=EMC^2 Glazier | Misc | 12 | October 25th 06 02:28 AM |
Cosmic Decreasing Gravity and the Expansion of the Universe | Louis Nielsen | Astronomy Misc | 4 | January 4th 05 11:03 AM |
Decreasing Gravity and the Expansion of the Earth | Louis Nielsen | Astronomy Misc | 4 | January 2nd 05 01:28 AM |
Accelerating Model of the Universe | azazel scratch | Misc | 3 | October 4th 04 02:36 AM |