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(necessary technical details) Explain very basics of tokamak physics
(necessary technical details) Explain very basics of tokamak physics

... refer to an embryonic or incomplete substance Similarly, golem is often used today in metaphor as an entity serving man under controlled conditions but hostile to him in others. ...
Creation of a magnetic plasmon polariton through strong coupling between... atom and the defect state in a defective multilayer microcavity
Creation of a magnetic plasmon polariton through strong coupling between... atom and the defect state in a defective multilayer microcavity

... to characterize the bulk metal properties. Namely, the metal permittivity in the infrared spectral range is given by ␧共␻兲 = 1 − ␻2p / 共␻2 + i␻␻␶兲, where ␻ p is the bulk plasma frequency, and ␻␶ is the relaxation rate. For gold, the characteristic frequencies fitted to experimental data are ␻ p = 1.3 ...
Last Time… - UW-Madison Department of Physics
Last Time… - UW-Madison Department of Physics

... Particle in box question A particle in a box has a mass m. Its energy is all kinetic = p2/2m. Just saw that momentum in state n is npo. It’s energy levels A. are equally spaced everywhere B. get farther apart at higher energy C. get closer together at higher energy. ...
Electromagnetic Induction
Electromagnetic Induction

... Southern Polytechnic State University ...
py354-final-121502
py354-final-121502

... This is a closed book exam. Any formulas you are likely to need, and would have trouble remembering are provided on the back page. Please do not use formulas or expressions stored in your calculators. Please write all your work in the space provided, including calculations and answers. Please circle ...
Modeling of scattering and depolarizing electro
Modeling of scattering and depolarizing electro

Chp9PertubationTimeDep
Chp9PertubationTimeDep

1-17 The Universal Law of Gravitation
1-17 The Universal Law of Gravitation

... Consider an object released from rest an entire moon’s diameter above the surface of the moon. Suppose you are asked to calculate the speed with which the object hits the moon. This problem typifies the kind of problem in which students use the universal law of gravitation to get the force exerted o ...
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1302lab6 - UMN Physics home

Grof, Jung, and the Quantum Vacuum
Grof, Jung, and the Quantum Vacuum

... Relevant work began in the 1970s, when Russell Targ and Harold Puthoff carried out some of the best known experiments on subtle connections among distant subjects in regard to the transference of thoughts and images. They examined the possibility of telepathic transmission between individuals, one ...
Poynting Paradox
Poynting Paradox

Deflection switching of a laser beam by the Pockels effect of water
Deflection switching of a laser beam by the Pockels effect of water

... measurement and analyzing methods above, the magnitude of the Pockels constants is reliably determined. However, it was not experimentally proved whether the refractive index change occurs completely within a few nanometer-thick EDL because the probing light is normally incident on the electrode sur ...
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Chapter Nine Radiation

... wave, charges in the scatterer will be set into some sort of coherent motion1 and these moving charges will produce radiation, called the scattered wave. Hence scattering phenomena are closely related to radiation phenomena. Diffraction of electromagnetic waves is similar. One starts with a wave in ...
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OpenFOAM Simulation for Electromagnetic Problems

... Based on the Maxwell equations, two different formulations (the A-V formulation and the A-J formulation) are derived to solve magnetrostatic field problems. Formulations are compiled manually into OpenFOAM solvers according to mathematic models by specific program codes. Furthermore, force calculati ...
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Macroscopic electric field and osmotic pressure in ultracentrifugal

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Measurement of the transverse electric field profile of light by a self

... that the general method in Ref [1]. is classical, it will only admit a quantum description in most systems (e.g. if applied to atomic orbitals). Conceptually the classical analog can be viewed as a way of extracting a measurement of the transverse electric field profile (TEFP) of a beam of light by ...
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... South Seeking Magnetic Poles, and like poles (i.e., N-N or S-S poles) repulse. One of the consequences of this is the peculiar situation we have with respect to the earth's magnetic field. 2.) By definition, the North Seeking Magnetic Pole of a compass points toward the northern geographic region of ...
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Dielectric Polarization

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PSE4_Lecture_2_Ch21

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Spin-orbit coupling

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Measurement of the electric field radiated by electrostatic discharges
Measurement of the electric field radiated by electrostatic discharges

a<x<a
a

... anymore. The energy is said to be quantized. This is characteristic of boundstate problems in quantum mechanics, where a particle is localized in a finite region of space. ...
13361_2011_210400501_MOESM1_ESM
13361_2011_210400501_MOESM1_ESM

CHARACTERIZATION OF THE SEQUENTIAL PRODUCT ON
CHARACTERIZATION OF THE SEQUENTIAL PRODUCT ON

< 1 ... 174 175 176 177 178 179 180 181 182 ... 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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