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Mutual Inductance
Mutual Inductance

... The emf induced in the secondary coil may now be calculated using Faraday’s law: ...
Critical Nuclear Charges for N-Electron Atoms
Critical Nuclear Charges for N-Electron Atoms

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The Casimir Effect 1 Introduction
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... which is the minimum oscillation frequency the electrons in the conductor can support. Below the plasma frequency, the conductor acts as a reactive medium and reflects electromagnetic waves giving rise to the boundary conditions discussed above. Above the plasma frequency, however, the electrons ar ...
Below is a list of topics that you should know to do well on the first test
Below is a list of topics that you should know to do well on the first test

... How to calculate the electric potential using the potential energy, the electric field, and from point charges (page 522 has the equations to use for each); 2, 8, 9, ...
When do particles follow field lines?
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... 2 objects with same property repel each other 2 objects with different properties attract each other both properties are always created together Benjamin Franklin: kinds of charges are positive and negative by convention, negative charge associated with amber Conservation of Charge: The algebraic su ...
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Low frequency fields

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Lect11

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Exam3_T133

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Revision of Electromagnetic Theory Lecture 2

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Magnetically Induced Reconstruction of the Ground State in a Few-Electron...

... The basics of Coulomb blockade (CB) phenomena can be understood within the so-called “orthodox theory” [1]. In this theory, electron-electron interactions are hidden in the charging energy, and the electrostatic coupling is assumed to be independent of the nature of the ground state, namely, on the ...
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Electro-Statics Think then MC

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Ch16CTb

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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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