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Questions 25 – 26
Questions 25 – 26

... *42. The electric field of two long coaxial cylinders is represented by lines of force as shown above. The charge on the inner cylinder is +Q. The charge on the outer cylinder is (A) +3Q (B) +Q (C) 0 (D) – Q (E) –3 Q 43. An isolated capacitor with air between its plates has a potential difference Vo ...
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... Alfvén waves in the fluid-kinetic simulations would be accompanied by bursts of accelerated electrons. A particle-in-cell (PIC) simulation was used by Clark and Seyler [1999] in proposing that nonlinear inertial Alfvén waves in the electrostatic limit are capable of producing suprathermal electron b ...
Peer-reviewed Article PDF
Peer-reviewed Article PDF

... and magnetic fields [41], unfortunately the shape of this wave have been mixed with semi-circle water waves generated in pond, interpreted as synonymous to magnetic wave [26], as shown in Figure 1A; but since it was discovered that, the electric field (E-F) produced in series of timelapse photograph ...
1.2 Single Particle Kinematics
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CHAPTER 20: Magnetism Answers to Questions
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... © 2005 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This material is protected under all copyr ight laws as they currently exist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher. ...
Document
Document

... © 2005 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This material is protected under all copyright laws as they currently exist. No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher. ...
2 Equipotential and Electric Field Mapping Experiment
2 Equipotential and Electric Field Mapping Experiment

... That is, work is equal to the force F exerted times the distance Δs over which that force was exerted. This formula is pretty easy when the force is constant, like if you were pushing a sled at a constant velocity across a uniform surface (with constant friction). The force that you exert at any loc ...
Path Integrals in Quantum Mechanics
Path Integrals in Quantum Mechanics

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SPLIT-FIELD FINITE-DIFFERENCE TIME-DOMAIN SCHEME FOR KERR-TYPE NONLINEAR PERIODIC MEDIA Jorge Franc´
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... Three objects are brought close to one another, two at a time. When objects A and B are brought together, they attract. When objects B and C are brought together, they repel. Which of the following are necessarily true? ...
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Quantum Faraday effect in graphene within relativistic Dirac model

November 2012 exam
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... (a) For the circuit shown above, with the directions of the currents chosen as shown, obtain three equations from which i1 , i2 and i3 can be determined. (DO NOT SOLVE FOR i1 , i2 , and i3 .) ...
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... In 1964, Solymar and Ash [1] published a one-dimensional analysis of an n-type semiconductor traveling wave amplifier predicting high gain per centimeter. They assumed a single species of charge carrier with infinite recombination lifetime obtaining a characteristic equation for the interaction that ...
Armin Scrinzi
Armin Scrinzi

... is not available to the present day. The formulae are deliberately not quoted here. They all are accurate “to exponential accuracy”, i.e. the exponential dependence on field and binding energy is reproduced correctly (but near trivially). This is the use that is made of them in practice. ...
< 1 ... 167 168 169 170 171 172 173 174 175 ... 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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