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Magnetic Fields
Magnetic Fields

... 12. An alpha particle travel through a magnetic field of 4.22 X 10-1 T perpendicular to the field. If the radius of the arc of the deflected particles is 1.50x10-3 m what is the speed of the particles? (3.05x104 m/s) 13. A proton travels through a magnetic field at a speed of 5.40x105 m/s perpendic ...
Homework No. 04 (2014 Fall) PHYS 320: Electricity and Magnetism I
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... 2πε0 r where r is now the radial vector transverse to the axis of the cylinder. (b) Plot the magnitude of the electric field as a function of r. (c) Rewrite your results for the case when the solid cylinder is a perfect conductor? (d) Rewrite your results for the case of a uniformly charged hollow c ...
Electric Fields
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Topological Phases of matter - Harvard Condensed Matter Theory

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Homework-Biot-Savart.. - University of Colorado Boulder
Homework-Biot-Savart.. - University of Colorado Boulder

... B) How is the mass m related to the known quantities q, E, B, and s? (Gravity can be ignored since it is very weak compared to the forces due to E and B.) Given the geometry shown, will this spectrometer work for + charges only, – charges only, or both + or – charges? Assigned in FA08 ...
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14 - Basic Theory of Nuclear Magnetic Resonance

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... EVALUATE: The positively charged ring attracts the negatively charged electron and accelerates it. The electron has its maximum speed at this point. When the electron moves past the center of the ring the force on it is opposite to its motion and it slows down. ...
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The Effect of an Ocean on Magnetic Diurnal Variations

... where N is the frequency of the inducing field in cycles per day. We have obtained solutions of (9) and (11) for the 24, 12, 8 and 6 hr harmonics. Figures I and z give the induced horizontal magnetic field Variations and the total vertical magnetic field variations corresponding to these solutions w ...
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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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