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Date: 8/24/2011 12:52:00 PM
From Authorid: 5301
...can you fix a warp drive?  |
Date: 8/24/2011 12:56:00 PM
From Authorid: 33286
I am having problems with my flux capacitor...  |
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Date: 8/24/2011 1:00:00 PM
From Authorid: 5301
...Hack...are you using a rosin based flux or acid base? |
Date: 8/24/2011 1:01:00 PM
From Authorid: 62993
Did I just get into thrown into Star Trek?  |
Date: 8/24/2011 1:05:00 PM
From Authorid: 64365
ya got it wrong, Hekler...it's a resin based flux...the acid one is called a reflux  |
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Date: 8/24/2011 1:08:00 PM ( Admin )
I was thinking along similar lines, however, did you consider... A stochastic model is derived to predict the turbulent torque produced by a swirling flow. It is a simple Langevin process, with a colored noise. Using the unified colored noise approximation, we derive analytically the PDF of the fluctuations of injected power in two forcing regimes: constant angular velocity or constant applied torque. In the limit of small velocity fluctuations and vanishing inertia, we predict that the injected power fluctuates twice less in the case of constant torque than in the case of constant angular velocity forcing. The model is further tested against experimental data in a von Karman device filled with water. It is shown to allow for a parameter-free prediction of the PDF of power fluctuations in the case where the forcing is made at constant torque. A physical interpretation of our model is finally given, using a quasi-linear model of turbulence. We obtain an exact analytic solution of the equation of motion for a dye laser with a fluctuating pump parameter of finite correlation time. The exact solution is compared with recent experimental results on the intensity fluctuations of a dye laser. We also obtain a favorable comparison of the experiments to the results obtained from an approximate Fokker--Planck description of the laser. We also investigate the 1/N expansion proposed recently as a strategy to include quantum fluctuation effects in the nonrelativistic, attractive Fermi gas at and near unitarity. We extend the previous results by calculating the next-to-leading order corrections to the critical temperature along the whole BCS-BEC crossover. We demonstrate explicitly that the extrapolation from the mean-field approximation, based on the $1/N$ expansion, provides a useful approximation scheme only on the BCS side of the crossover. We then apply the technique to the study of strongly interacting relativistic many-fermion systems. Having in mind the application to color superconductivity in cold dense quark matter, we develop, within a simple model, a formalism suitable to compare the effects of order parameter fluctuations in phases with different pairing patterns. Our main conclusion is that the relative correction to the critical temperature is to a good accuracy proportional to the mean-field ratio of the critical temperature and the chemical potential. As a consequence, it is significant even rather deep in the BCS regime, where phenomenologically interesting values of the quark-quark coupling are expected. Possible impact on the phase diagram of color-superconducting quark matter is discussed. Potentials between static quarks and antiquarks from a few lowest representations were evaluated in numerical simulations of 4-dimensional pure G$_2$ lattice gauge theory at various couplings. The obtained potentials are linearly rising at intermediate distances and their string tensions exhibit (approximate) Casimir scaling. This result is in accordance with a model of the vacuum of non-Abelian gauge theories with a domain structure, in which the (color) magnetic flux randomly fluctuates within a domain, but the total flux in each domain is quantized in units of the gauge group center. The internal configuration of the color-carrying degrees of freedom of an ultrarelativistic hadron is frozen by Lorentz time dilation. When the spatial extent of the configuration is small, the hadron interacts weakly with other hadrons - the phenomenon of color transparency - since the color fields generated by the overall color neutral components nearly cancel. The hadron experiences only weak color-dipole interactions for small configurations. similarly, when the color configuration of the hadron is large it interacts more strongly than average - a color opacity. Such varying interactions are described by fluctuations in the interaction cross-sections of hadrons, which are intimately related of the phenomena of inelastic shadowing and diffractive dissociation. This connection allows on the deduce information on cross-section fluctuations from measurements of these phenomena. Cross-section fluctuations give rise to important fluctuations in observed quantities, such as multiplicity and transverse energy, produced in ultrarelativistic heavy-ion collisions. There are those that can present a study of the shear modulus of the crystalline color superconducting phase of quark matter, showing that this phase of dense, but not asymptotically dense, quark matter responds to shear stress as a very rigid solid. This phase is characterized by a gap parameter $\\Delta$ that is periodically modulated in space and therefore spontaneously breaks translational invariance. We derive the effective action for the phonon fields that describe space- and time-dependent fluctuations of the crystal structure formed by $\\Delta$, and obtain the shear modulus from the coefficients of the spatial derivative terms. Within a Ginzburg-Landau approximation, we find shear moduli which are 20 to 1000 times larger than those of neutron star crusts. This phase of matter is thus more rigid than any known material in the universe, but at the same time the crystalline color superconducting phase is also superfluid. These properties raise the possibility that the presence of this phase within neutron stars may have distinct implications for their phenomenology. For example, (some) pulsar glitches may originate in crystalline superconducting neutron star cores. Did I over simplify that? Any who, I have to get back to sorting my MM's. Perfect, not perfect but orange, blue defiantly has to be dealt with along with green-ultraviolet which is relatively low compared to high energy red-infrared. The disappearence of my hyperbolic light scattering mirror slows down the sorting process considerably. -Rad.. |
Date: 8/24/2011 1:09:00 PM
From Authorid: 34663
Got through the first sentence and nearly fell asleep, lol  |
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Date: 8/24/2011 1:24:00 PM
From Authorid: 33286
Heckler... did I say flux? I meant FLAX... it is going right through me and I need it to stop, so I figured my capacitor was broken |
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Date: 8/24/2011 1:25:00 PM
From Authorid: 34663
just curious, aside from Rad does anyone know what this post is talking about and can someone put it into grade school terms for me so I can understand, lol |
Date: 8/24/2011 1:58:00 PM
From Authorid: 44960
Where is Seedot when we need him!!   |
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Date: 8/24/2011 3:50:00 PM
From Authorid: 33286
I think Lewis Carroll said it best... Twas brillig, and the slithy toves Did gyre and gimble in the wabe: All mimsy were the borogoves, And the mome raths outgrabe. "Beware the Jabberwock, my son! The jaws that bite, the claws that catch! Beware the Jubjub bird, and shun The frumious Bandersnatch!" He took his vorpal sword in hand: Long time the manxome foe he sought -- So rested he by the Tumtum tree, And stood awhile in thought. And, as in uffish thought he stood, The Jabberwock, with eyes of flame, Came whiffling through the tulgey wood, And burbled as it came! One, two! One, two! And through and through The vorpal blade went snicker-snack! He left it dead, and with its head He went galumphing back. "And, has thou slain the Jabberwock? Come to my arms, my beamish boy! O frabjous day! Callooh! Callay!' He chortled in his joy. `Twas brillig, and the slithy toves Did gyre and gimble in the wabe; All mimsy were the borogoves, And the mome raths outgrabe. |
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Date: 8/24/2011 4:10:00 PM
From Authorid: 10722
Tiptoe through the window By the window, that is where I'll be Come tiptoe through the tulips with me. Oh, tiptoe from the garden By the garden of the willow tree And tiptoe through the tulips with me. Knee deep in flowers we'll stray We'll keep the showers away And if I kiss you in the garden, in the moonlight Will you pardon me? And tiptoe through the tulips with me.  |
Date: 8/24/2011 5:15:00 PM
From Authorid: 3680
Will someone please pass the jelly!  |
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Date: 8/24/2011 5:38:00 PM
From Authorid: 33286
here you go D.R http://www.youtube.com/watch?v=Z3ZAGBL6UBA&ob=av3e |
| Date: 8/24/2011 9:08:00 PM ( SD-Admin ) This was Interesting. Post on |
| Date: 8/24/2011 9:09:00 PM ( SD-Admin ) I really like this Post! I love the comments |
Date: 8/25/2011 12:47:00 PM
From Authorid: 63258
Agreed....  |
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62821 Category:(Science) Created:(8/24/2011 12:33:00 PM)