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Maxwell`s Equations for Electricity and Magnetism
Maxwell`s Equations for Electricity and Magnetism

... where µ0 is a physical constant (the permeability of vacuum, 4π × 10−7 henry/meter). Note the similarity to Coulomb’s Law (2): like the electric field, the magnetic field is inversely proportional to the square of the distance. Now we consider an infinite straight wire carrying current I, and calcul ...
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Magnetism - Cuero ISD

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Sep. 28 - Bryn Mawr College

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Induction and Inductance - Mansfield Public Schools

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The Weird World of Quantum Information

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Motors and Generators

... • A strong current is suddenly switched on in a wire, but no force acts on the wire. Can you conclude that there is no magnetic field at the location of the wire? • No. It is possible that there is a magnetic field but that it is parallel to the wire. There is no force when a magnetic field and a wi ...
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Physics 2401 Summer 2, 2012 Exam 1

... ke = 9.0x109 Nm2/C2, m(proton) = 1.67x10-27 kg. n = nano = 10 , µ = micro = 10-6, m = milli = 10-3 Put your answers on the orange scantron which you brought. Write down and bubble in (correctly) your R# before you do anything else. All questions are weighted equally. 1. Two point charges which are a ...
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The Aharonov-Bohm Magnetic Field is Not Zero and the Electron Spirals
The Aharonov-Bohm Magnetic Field is Not Zero and the Electron Spirals

p3 unit2 sco
p3 unit2 sco

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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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