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L2 Gauss
L2 Gauss

force on a current in a magnetic field
force on a current in a magnetic field

Unruh Effect in Closed String Theory
Unruh Effect in Closed String Theory

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... plasma motion and magnetic topology is conserved. This sets strong limitations on the accessible dynamical states. Large-scale magnetic flux tubes, which are strongly stretched out by the plasma pressure, as for instance observed in PLANETARY MAGNETOSPHERES or in stellar CORONAs, would be unable to ...
ELECTRIC POTENTIAL ENERGY -Chapter 19
ELECTRIC POTENTIAL ENERGY -Chapter 19

... the bottom plate so that each positive charge lines up with a negative charge directly across from it. This arrangement of charges creates electric field lines which are directed from the positive charges to the negative charges and are uniformly spaced to produce a uniform (constant) electric field ...
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... coupling to the nuclear spin bath and estimates decoherence time from this source (for details, see ESI†).22 Note that this approximation neglects other decoherence sources; therefore, it only provides an upper bound for the decoherence time. Nevertheless, it is a useful tool to provide a starting p ...
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... For mineral oil, T1 and T2 were the same value at 21 ms. For glycerin, T1 was 41 ms and T2 was 44 ms. According to this data, mineral oil has returns to equilibrium more rapidly than glycerin. The values for mineral oil are inconsistent with those found in literature2,3 in which T2 of mineral oil (1 ...
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Deviations of Geomagnetic Field and Hydromagnetic Characteristics

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A short Introduction to Feynman Diagrams

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Rotation of electromagnetic fields and the nature of optical angular

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14:TRANSDUCERS

if on the Internet, Press  on your browser to
if on the Internet, Press on your browser to

... Some physicists believe that this conscious selection takes place in microtubules which are a feature inside every cell. Also, some physicists are proposing that the conscious selection is informed by information from both Past and Future. If these concepts are valid, they would have some very wide ...
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Electric Potential Practice Problems

The impact of hyperfine interaction on the charge radius of Protons
The impact of hyperfine interaction on the charge radius of Protons

Tuesday, Sept. 13, 2011
Tuesday, Sept. 13, 2011

...  E  dA   Eext   Ei  dA   0   0 The enclosed charge! • The value of the flux depends on the charge enclosed in the surface!!  Gauss’ law. ...
NIFS-886 (pdf file)
NIFS-886 (pdf file)

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Aharonov–Bohm effect

The Aharonov–Bohm effect, sometimes called the Ehrenberg–Siday–Aharonov–Bohm effect, is a quantum mechanical phenomenon in which an electrically charged particle is affected by an electromagnetic field (E, B), despite being confined to a region in which both the magnetic field B and electric field E are zero. The underlying mechanism is the coupling of the electromagnetic potential with the complex phase of a charged particle's wavefunction, and the Aharonov–Bohm effect is accordingly illustrated by interference experiments.The most commonly described case, sometimes called the Aharonov–Bohm solenoid effect, takes place when the wave function of a charged particle passing around a long solenoid experiences a phase shift as a result of the enclosed magnetic field, despite the magnetic field being negligible in the region through which the particle passes and the particle's wavefunction being negligible inside the solenoid. This phase shift has been observed experimentally. There are also magnetic Aharonov–Bohm effects on bound energies and scattering cross sections, but these cases have not been experimentally tested. An electric Aharonov–Bohm phenomenon was also predicted, in which a charged particle is affected by regions with different electrical potentials but zero electric field, but this has no experimental confirmation yet. A separate ""molecular"" Aharonov–Bohm effect was proposed for nuclear motion in multiply connected regions, but this has been argued to be a different kind of geometric phase as it is ""neither nonlocal nor topological"", depending only on local quantities along the nuclear path.Werner Ehrenberg and Raymond E. Siday first predicted the effect in 1949, and similar effects were later published by Yakir Aharonov and David Bohm in 1959. After publication of the 1959 paper, Bohm was informed of Ehrenberg and Siday's work, which was acknowledged and credited in Bohm and Aharonov's subsequent 1961 paper.Subsequently, the effect was confirmed experimentally by several authors; a general review can be found in Peshkin and Tonomura (1989).
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