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Waves, Fields & Nuclear Energy
Waves, Fields & Nuclear Energy

January 2010
January 2010

... A solid metallic sphere of radius a has finite conductivity, carries no net electric charge, and is free to rotate without friction about a vertical axis through its center. The region outside the sphere is ~ 0 parallel to the axis. vacuum. There is a uniform magnetic field with flux density B The s ...
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... 2-An ion with a charge of + 3.2 × 10–19 C is in a region where a uniform electric field of magnitude 5 × 104 V/m is perpendicular to a uniform magnetic field of magnitude 0.8 T. If its acceleration is zero what its speed. 3-An electron (charge = –1.6 × 10–19C) is moving at 3 × 105 m/s in the positiv ...
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chapter 29-30 quiz

... 2-An ion with a charge of + 3.2 × 10–19 C is in a region where a uniform electric field of magnitude 5 × 104 V/m is perpendicular to a uniform magnetic field of magnitude 0.8 T. If its acceleration is zero what its speed. 3-An electron (charge = –1.6 × 10–19C) is moving at 3 × 105 m/s in the positiv ...
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TT 35: Low-Dimensional Systems: 2D - Theory - DPG

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Presentation - El blog del Séneca

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... 1. A compass that has been calibrated in the Earth’s magnetic field is laced near the end of a permanent bar magnet, and points away from that end of the magnet. It can be concluded that the end of the magnet (a) acts as a north magnetic pole, (b) acts as a south magnetic pole, (c) you can’t conclud ...
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1. The figure shows a uniform magnetic field that is normal

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< 1 ... 608 609 610 611 612 613 614 615 616 ... 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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