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Yousuf Khan wrote:
Sounds like he's talking about the Aether Theory without actually mentioning the Aether here. Technology Review: Blogs: arXiv blog: The Clue That Could Explain The Fly-By Anomalies "Last year, we looked at an idea from Stephen Adler at Princeton University, that suggested the change in velocity could caused by collisions between the spacecraft and particles of dark matter. Adler even calculated the kind of distribution of dark matter particles that would explain the observed changes in velocity--a kind of halo of them around Earth. " http://www.technologyreview.com/blog/arxiv/24232/?a=f Yousuf Khan By hypothesis and definition dark matter does not interact except by gravitation. Do neutrinos slow spacecraft? -- Uncle Al http://www.mazepath.com/uncleal/ (Toxic URL! Unsafe for children and most mammals) http://www.mazepath.com/uncleal/lajos.htm#a2 |
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In sci.astro Uncle Al wrote:
By hypothesis and definition dark matter does not interact except by gravitation. Not true. By hypothesis, dark matter interacts weakly, but there is certainly no requirement of no nongravitational interaction. In fact, popular candidates (lightest supersymmetric particle, axions) certainly do have nongravitational interactions. In fact, a major experimental effort is going into searches for dark matter through such interactions. Steve Carlip |
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On Oct 14, 8:27*am, wrote:
In sci.astro Uncle Al wrote: By hypothesis and definition dark matter does not interact except by gravitation. * Not true. *By hypothesis, dark matter interacts weakly, but there is certainly no requirement of no nongravitational interaction. For Dark Matter as WIMPs, this is true. But the Bullet Cluster obviates such weakly interacting Dark Matter, doesn't it? The visible matter is pretty hot, so maybe we cannot evaluate how much normal matter is there... *In fact, popular candidates (lightest supersymmetric particle, axions) certainly do have nongravitational interactions. *In fact, a major experimental effort is going into searches for dark matter through such interactions. Isn't that a bit like searching for a lost item under a streetlight, even if we did not lose the item there, because we can at least see? David A. Smith |
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carlip-nospam wrote on Wed, 14 Oct 2009 15:27:19 +0000:
In sci.astro Uncle Al wrote: By hypothesis and definition dark matter does not interact except by gravitation. Not true. By hypothesis, dark matter interacts weakly, but there is certainly no requirement of no nongravitational interaction. In fact, popular candidates (lightest supersymmetric particle, axions) certainly do have nongravitational interactions. In fact, a major experimental effort is going into searches for dark matter through such interactions. What a waste of time and money! Steve Carlip -- http://www.canonicalscience.org/ BLOG: http://www.canonicalscience.org/en/p...encetoday.html |
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Uncle Al wrote:
[...] Uncle Al calls "bull****" on undetected matter in space in sufficient quantities to detectably alter local orbits, by collision cross-section or by naked gravitation. If somebody comes up with a reproducible lab signal (not the Italian stuff), Uncle Al will apologize. Correct. Any dark matter sufficiently dense to alter spacecraft orbits (and that bar is pretty high to begin with) will do...what to planetary and lunar orbits? The answer is an exercise for the reader. |
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Dear eric gisse:
On Oct 14, 9:01*pm, eric gisse wrote: Uncle Al wrote: [...] Uncle Al calls "bull****" on undetected matter in space in sufficient quantities to detectably alter local orbits, by collision cross-section or by naked gravitation. *If somebody comes up with a reproducible lab signal (not the Italian stuff), Uncle Al will apologize. Correct. Any dark matter sufficiently dense to alter spacecraft orbits (and that bar is pretty high to begin with) will do...what to planetary and lunar orbits? The answer is an exercise for the reader. The effect is a function of distance from the boost body, and if it resolved to similar "viscosity" models, would be on the order of v^2. Since inside the Roche limit is out for rocky bodies, we are left with ~1 km/sec for our Moon, vs. ~7.5 km/sec for a satellite. The problem is, an orbit encounters the "two kinds" of Dark Matter, the stuff "in front" and the stuff "behind", so it should average to (perhaps) zero net effect. But this too should be detectable. Were it not horse manure. David A. Smith |
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In sci.astro eric gisse wrote:
Any dark matter sufficiently dense to alter spacecraft orbits (and that bar is pretty high to begin with) will do...what to planetary and lunar orbits? Not necessarily very much. The interactions aren't gravitational -- there's no principle of equivalence at work here -- and the acceleration due to drag can be much greater for a small object than a large one. Adler's proposal is probably not what's really happening -- he himself says only that "the dark matter scenario is not currently ruled out, but requires dark matter to be non-self-annihilating, with the dark matter scattering cross section on nucleons much larger, and the dark matter mass much lighter, than usually assumed." But he's not an idiot, and he has looked at whether the model would have any other observable effects on Solar System measurements. (He is, in particular, looking at a model in which dark matter is gravitationally bound to the Earth and other planets. This would make the density near the Earth much higher than the average Solar System density.) I'm not arguing that Adler is right. But this is nontrivial stuff, and can't be dismissed by hand-waving; you have to really do the math. Steve Carlip |
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Uncle Al wrote:
NO DETECTIONS. Gravity Probe B (such as it was) showed no anomaly. in response: The Gravity Probe B continued data analysis with KACST? appears to further confirm Einstein's General Relativity Frame-dragging theory. http://einstein.stanford.edu/RESOURC...ons-index.html I would suggest another perspective which would make the study of Gravity Probe B very important in the context of analyzing the anomalous "polhode?" effect in terms of the universal 'dark energy' a concept which was not known at the Gravity Probe B conception. http://arxiv.org/abs/physics/9905007 In this paper (Table 2.4.1), there is a correlation which indicates that substantially all (~70%) of the universe (as currently depicted by 'dark energy' at 8.11E-16 K) has an oscillating period of 2.96E4 sec or 8.22 hours (frequency of 3.38E-5 hz). The data presented in the seminar, http://einstein.stanford.edu/RESOURC...ons-index.html indicates this universal dark energy frequency of 3.38E-5 hz is be harmonically related to seminar presented Asymtotic Polhode frequencies. http://einstein.stanford.edu/RESOURC...ons-index.html July 8, 2009 • Stanford University HEPL Seminar Polhode Motion, Trapped Flux, and the GP-B Science Data Analysis Alex Silbergleit, John Conklin and the Polhode/Trapped Flux Mapping Task Team 2.4 Dissipation Modeling: Products 1. Asymptotic Polhode Period and Dissipation Time | Asymptotic Asymptotic Asymptotic Asymptotic | Polhode Polhode Polhode Polhode | Period frequency harmonic harmonic | (hours) (Hertz) deviation gyro 1 0.867 3.20E-04 9 1.05 gyro 3 1.529 1.82E-04 5 1.08 gyro 2 2.581 1.08E-04 3 1.06 gyro 4 4.137 6.71E-05 2 0.99 universe 8.22 3.38E-05 1 1.00 The hypothesis would be that this residual asymptotic frequency is not totally a polhode frequency but partially an induced gyro frequency, representing an harmonic of the external universe dark energy Further, the hypothesis would be that the Gravity Probe B gyroscope niobium superconductor Cooper mass (5.79E-10 g) is subject to gravitational tidal oscillation (induced gyro frequency) by the substantial universe mass (dark energy/c^2) with density 6.38E-30 g/cc. The Gravity Probe B gyroscope niobium superconductor Cooper mass is calculated to be 5.79E-10 g as follows: niobium critical temperature (Tc) = 8 K niobium niobium thickness 1270 nm gyroscope diameter 3.81 cm (1.5 inch) niobium volume pi*3.81*3.81*1.27E-6 = 5.79E-5 cm3 http://arxiv.org/abs/physics/9905007 Table 2.9.1 Cooper Pair density is 1E-5 g/cc Therefore Cooper Pair Mass = 5.79E-10 g This Cooper Pair Mass may be characterized in a somewhat fluid form subject to dimensional distortion. The continued hypothesis would be that the Cooper Pair mass of 5.79E-10 g contained in Gravity Probe B gyroscope niobium superconductor gravitationally tidally oscillates with the universe mass at a frequency of 3.38E-05 hertz and harmonics as animated in: http://einstein.stanford.edu/Media/P...animation.html approaching an asymptotic value in step with oscillating universe 'dark energy'. Similar frequencies have been noted throughout the universe and in particular the power spectra if Active Galactic Nuclei (AGN) (Seyferts and Blazars) http://arxiv.org/abs/astro-ph/0101542 which perhaps have equivalent low densities (as niobium Cooper pair densities) subject to such gravitational interaction with the oscillating universe 'dark energy'. Also, such frequencies have been noted in the earth's upper atmosphere under the name 'Temporal variability of the telluric sodium layer'. http://arxiv.org/abs/astro-ph/0609307 Calculations indicate that such an atmospheric tidal effect by oscillating universe 'dark energy' would affect flyby spacecraft such as observed. Such an effect would not be observed in flybys of non atmospheric celestial bodies. In conclusion, the Gravity Probe B may be a measure of Einstein's General Relativity but perhaps as importantly, a measure of the universe oscillating 'dark energy' providing a more fundamental understanding of its nature. Richard D. Saam |
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