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Ch 26 Lecture
Ch 26 Lecture

theoretical investigation of dielectrophoresis and electrophoresis as
theoretical investigation of dielectrophoresis and electrophoresis as

... particle with a radius of 3 µm. It is observed from this model that a silver microparticle with a radius of 3 µm moving in a helium medium with the bulk velocity of 0.021 ms−1 and subjected to a dielectrophoretic force only deflect an amount of 0.52039 nm and 4.49882 nm in the x - and z -directions ...
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... which leads to a many-body behavior governed by 2D physics. This is for example the case in materials like graphene or layered superconductors, where the electron gas is confined in two-dimensional planes [Nor11, Jos13]. Although axially excited quantum states still exist, they are not populated sin ...
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... 8-4. Comparison of HEMP and lightning. HEMP-induced surge currents on overhead transmission lines are similar to, but not exactly the same as, lightning-induced surges. Table 8-1 compares worst-case surges. From the numerical values, it could be inferred that lightning is a more serious threat. The ...
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... “fictitious charge layers” throughout the interior of the cylinder. The charge layers do not have a significant effect until a relative permittivity greater than approximately 10 is used, causing an unstable solution. The fictitious charge layers can be avoided with the use of ...
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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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