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1 Exam 1: Exam 1: Magnetic Field Bar Magnets
1 Exam 1: Exam 1: Magnetic Field Bar Magnets

January 2001
January 2001

printable version - Gosford Hill School
printable version - Gosford Hill School

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Physics 213—Problem Set 10—Solutions Fall 1997
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... plane of incidence, which is more precisely defined as the plane spanned by the incident k vector and the normal to the surface. With E lying in the plane of incidence, the wave is said to have parallel polarization or to be p-polarized (E is parallel to the incidence plane). Note that although H i ...
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Basic MR Imaging (MRI) and MR spectroscopy (MRS)

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FinalExam02f_solution

... current in the horizontal rail since the current is small, i.e. it is not a rail gun). a) The current i in the wire (from the source G) is sitting in the magnetic field B, resulting in force towards the left. The wire is accelerating towards the left. As the wire starts to move left, a current is in ...
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A: The magnetic field cancels outside!

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Static-Electricity-and-Fields-Test-Study-Guide

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Magnets And Magnetic Fields

εε ε ε ε
εε ε ε ε

< 1 ... 606 607 608 609 610 611 612 613 614 ... 661 >

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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