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Electromagnetic Induction
Electromagnetic Induction

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ElectroMagnetic Induction

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... ratio of the half angular widths of the first secondary maxima, in the two cases, be also equal to q? ...
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... radius to high speeds. The charged particles are subjected to both an electric field and a magnetic field. One of these fields increases the speed of the particles, and the other field holds them in a circular path. Which field performs which function? 7. A magnetic field can deflect a beam of elect ...
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... is free to take either spin state, however if two electrons occupy the orbital, they must take opposing spin states and thus their magnetic moments cancel out. The total spin state of the atom can then be determined by considering the net spin of the constituent electrons. For example, hydrogen has ...
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Topic 4 - Introduction to Quantum Theory

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87essay - PLK Vicwood KT Chong Sixth Form College

... Diffraction is a bending of the waves around the edge of obstacles. there are centres of disturbance on the wave front in plane of obstacle, such as P, and these send out waves (spherical) as shown propagating behind obstacle. (c) For observable diffraction the wavelength of the waves has to be comp ...
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Physics: Principles and Applications

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Physics: Principles and Applications

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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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