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PHY 2054 Fall 2012 Kumar/Mitselmakher Exam I
PHY 2054 Fall 2012 Kumar/Mitselmakher Exam I

... top vertex contains a charge (8, 32) nC. The two vertices at the base contain a charge of -4 nC.. Calculate tthe he magnitude (in N/C) and direction of the electric field at point P, the midpoint of the base. Answer (4.5,18), down Solution: Note here that the electric field due to the lower two nega ...
Slide 1
Slide 1

1m 12cm x =.12m 100cm F =BiLsinθ
1m 12cm x =.12m 100cm F =BiLsinθ

Paper
Paper

... they can share one beam). This implies that the synthetic magnetic field can now be chosen to be the same, to be opposite, or to be different for the two spin states. One option is to have zero synthetic magnetic field for one of the states. Atoms in this state can still tunnel along the tilt direct ...
Set1 - CBSE
Set1 - CBSE

Bose–Einstein condensation NEW PROBLEMS
Bose–Einstein condensation NEW PROBLEMS

... A. De Broglie wavelength and BEC In the semiclassical approximation at low density and high temperature, atoms are localized to wave packets with dimensions small compared to the average interatomic separation. The average de Broglie wavelength l 5 h/p, which is a quantum measure of delocalization o ...
Electrical Potential
Electrical Potential

Physics 51
Physics 51

Physics     Week 5(Sem. 2) Magnetism
Physics     Week 5(Sem. 2) Magnetism

... moving with a velocity of v through a magnetic field.   The vector of the magnetic field is labeled B, it is  assumed to be constant in magnitude and direction.  If  the charge moves parallel or antiparallel then the  charge experiences no magnetic field.  If, the charge  moves perpendicular to the  ...
Chapter 23 Electrical Potential
Chapter 23 Electrical Potential

... metal sphere that has a charge –Q. Sketch the electric field lines and equipotential surfaces for this system of charges. Picture the Problem The electric field lines, shown as solid lines, and the equipotential surfaces (intersecting the plane of the paper), shown as dashed lines, are sketched in t ...
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11 - The Left Hand RULES!!!

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Student Activity DOC

Use of Superconductors in the Excitation System of
Use of Superconductors in the Excitation System of

... In the mixed state, the magnetic field is able to penetrate inside the bulk of the superconductor. This penetration only exists in tiny tubes known as flux tubes (Figure II-4 (a)), which are surrounded by superconducting current vortices, as shown in Figure II-4 (b). The flux tubes are enclosed in a ...
Adobe Acrobat file () - Wayne State University Physics and
Adobe Acrobat file () - Wayne State University Physics and

... By a clever change to the rings and brushes of the ac generator, we can create a dc generator, that is, a generator where the polarity of the emf is always positive. The basic idea is to use a single split ring instead of two complete rings. The split ring is arranged so that, just as the emf is abo ...
Laser-dressed scattering of an attosecond electron wave
Laser-dressed scattering of an attosecond electron wave

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No Slide Title

07_Entanglement_in_nuclear_quadrupole_resonance_
07_Entanglement_in_nuclear_quadrupole_resonance_

... become the single most important theoretical paper in physics to appear since 1945; it was entitled On the Einstein Podolsky Rosen Paradox. • In 1964,John Bell showed that the predictions of quantum mechanics in the EPR thought experiment are significantly different from the predictions of a very br ...
Apprenticeship at the IBM Almaden Research Center
Apprenticeship at the IBM Almaden Research Center

Charge carriers transport properties in CdTe measured with
Charge carriers transport properties in CdTe measured with

Nature template - PC Word 97
Nature template - PC Word 97

... confinement respectively. The bias field is 0.75 G corresponding to a frequency of 2.1 MHz for a transition between the mJ = 1 and mJ = 0 states at the bottom of the trap. After evaporative cooling, we keep an RF knife on at constant frequency for 500 ms, then wait for 100 ms before switching off th ...
St_Pierre_2002 - Scientific and Clinical Applications of Magnetic
St_Pierre_2002 - Scientific and Clinical Applications of Magnetic

Gauss` Law
Gauss` Law

... Define E2 to be equal to the magnitude of the electric field at r = 1.4 cm when the charge on the outer shell (q2) is equal to 1.1 μC. Define Eo to be equal to the magnitude of the electric field at r = 1.4 cm if the charge on the outer shell (q2) were changed to 0. Compare E2 and Eo. E2 = Eo Since ...
CMS: Compact Muon Solenoid ATLAS: A Toroidal LHC ApparatuS
CMS: Compact Muon Solenoid ATLAS: A Toroidal LHC ApparatuS

PHet Simulation: Field of Dreams Purpose: To observe the electrical
PHet Simulation: Field of Dreams Purpose: To observe the electrical

< 1 ... 307 308 309 310 311 312 313 314 315 ... 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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