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Electricity and Magnets
Electricity and Magnets

Unit - SVCE
Unit - SVCE

... 1. To store charge 2. To store energy ...
Electric fields
Electric fields

12.2 Oersted`s Discovery
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... Oersted’s Experiment Before Oersted, many physicists had hypothesized that magnetic fields could be created by an electric current in a wire. Oersted hypothesized that the current would produce a magnetic field that radiated away from the wire. He tested his hypothesis with a compass held near a con ...
Modeling the Scattering by Small Holes
Modeling the Scattering by Small Holes

... Abstract— The scattering by a hole/aperture within a perfect electric conducing (PEC) plane is a classical electromagnetic problem. As is well known, this scattering can be formulated as the solution of an integral equation where the unknown aperture electric field (or equivalently the magnetic sour ...
Review: Magnetic Flux, EMF 20.3 Motional EMF Motional EMF
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... slip rings that rotate with the loop Connections to the external circuit are made by stationary brushes in contact with the slip rings ...
Faraday`s Law of Induction
Faraday`s Law of Induction

... • Faraday concluded that an electric current can be produced by a changing magnetic field. • A current cannot be produced by a steady magnetic field. • The current that is produced in the secondary circuit occurs for only an instant while the magnetic field through the secondary coil is changing. • ...
Revista Mexicana de Física . Darboux-deformed barriers
Revista Mexicana de Física . Darboux-deformed barriers

... T has a series of local maxima and minima. The maxima are reached for the values of E such that ∆ is minimum. These energies are known as transparencies because the particles travel trough the barrier zone as if they were free of interactions [33]. If 0 < ² = E < V0 , then q is pure imaginary, there ...
Transient induced molecular negative ions formed in cold electron
Transient induced molecular negative ions formed in cold electron

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... Present concepts for spintronic devices invoke the manipulation of spins by electric voltages or currents. This task is conceptually accomplished making use of spinorbit (SO) coupling which is a mechanism involving both electronic and spin properties: SO interaction is seen by the spin of an electro ...
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Lecture 14: Generalised angular momentum and electron spin

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Lab 2: Electric Fields – Coulomb Force at a Distance

... Lab 2: Electric Fields – Coulomb Force at a Distance Introduction The Coulomb force, Fc, between two charges is determined by their magnitude, q1 and q2, and position, r. The concept of an electric field E=Fc/q= C Q/r2, similar to a gravitational field g= 9.8 m/s = GM/re2, is helpful in solving prob ...
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Document

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1. The specific heat of lead is 0.030 cal/g ∙ °C. 300 g of lead shot at

Chapter 1: Lagrangian Mechanics
Chapter 1: Lagrangian Mechanics

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Megavolt Parallel Potentials Arising from Double

... dashed lines result from the absence of high time resolution data and the horizontal solid lines covered regions where there was data and no double layers. The steps in Fig. 3(c) indicate the potential jumps associated with the fewsecond durations of double-layer streams that involved 7000 double la ...
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17-6 Capacitors and Dielectrics

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1 nuclear fusion - a different approach.pages

Chapter 6: Electrostatics End of Chapter Questions
Chapter 6: Electrostatics End of Chapter Questions

< 1 ... 342 343 344 345 346 347 348 349 350 ... 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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