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Permission to make digital or hard copies of all or part of this work
Permission to make digital or hard copies of all or part of this work

Temperature gradients due to adiabatic plasma
Temperature gradients due to adiabatic plasma

Electromagnetic Wave Theory
Electromagnetic Wave Theory

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Internal forces in nondegenerate two-dimensional electron systems * C. Fang-Yen

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arXiv:0912.4058v1 [physics.atom

Surface field in an ensemble of superconducting spheres under
Surface field in an ensemble of superconducting spheres under

Electricity and Magnetism I (PHY 321) Gauss`s Law problems
Electricity and Magnetism I (PHY 321) Gauss`s Law problems

... where e is the charge of the proton and a0 is the Bohr radius. Find the electric field produced by the hydrogen atom at an arbitrary point in space. Express your answer in terms of e and a0 . Problem 10 Consider a long straight line charge with linear charge density λ. Choose a coordinate system and ...
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The Interaction of Radiation and Matter: Quantum

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Generators and Transformers

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Carbon nanotubes in electric and magnetic fields

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PHY481 Exam 1 NO books, notes, calculators, cell phones
PHY481 Exam 1 NO books, notes, calculators, cell phones

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The operation of a rotating magnetic machine is

Chapter 24 Capacitance, dielectrics and electric energy storage
Chapter 24 Capacitance, dielectrics and electric energy storage

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Why do particle clouds generate electric charges?

... Moon and to Mars9,10 , where charged dust degrades solar-cell viability and clings to spacesuits, limiting the lifetime of their joints11 . Several research groups have investigated mechanisms by which similar particles may charge one another, for example because of non-uniform heating12 , differenc ...
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Physics For Engineers and Scientists II

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Lecture 18: Antennas and interference

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Quantum mechanical spin and addition of angular momenta

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In uence of Magnetic Field on Dielectric Breakdown in Transformer

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the vlasov–poisson system with strong magnetic field

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An asymptotic preserving scheme for the Schrödinger equation in

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The Hall Effect and the Beauty and Challenges of Science

... field will in general contain contributions arising from temperature gradients and entering through the thermoelectric and thermomagnetic coefficients. Inasmuch as the usual theoretical relationships involving the Hall effect are based on isothermal conditions, we now have two choices: (a) d 0 measu ...
Electromagnetic Induction
Electromagnetic Induction

... Electromagnetic Induction ...
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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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