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Homework 4 A uniform electric field of magnitude E = 435 N/C makes
Homework 4 A uniform electric field of magnitude E = 435 N/C makes

Uniform Electric Fields and Potential Difference
Uniform Electric Fields and Potential Difference

... • compare, qualitatively, gravitational potential energy and electric potential energy. • define electric potential difference as a change in electric potential energy per unit of charge. • calculate the electric potential difference between two points in a uniform electric field. • explain, quantit ...
Forces and Fields.
Forces and Fields.

Document
Document

cond-mat/0601319 PDF
cond-mat/0601319 PDF

... The main point, however, is that the considered above gauge transformation does not fall under the known gauge transformations, neither the Lorentz gauge nor the Coulomb gauge [15], and cannot formally lead to the wave equation. Moreover, to have a wave process one should suppose that there exists a ...
1 Two identical current loops have currents I flowing in opposite
1 Two identical current loops have currents I flowing in opposite

03_E2_ws2_key
03_E2_ws2_key

em_motor_doc - School of Physics
em_motor_doc - School of Physics

PHYS 241 Exam Review
PHYS 241 Exam Review

PhET Simulation
PhET Simulation

Motors and Generators Syllabus
Motors and Generators Syllabus

... as coal, or use the energy of falling water to generate electricity on a large scale. Electricity is also relatively easy to distribute. Electricity authorities use high-voltage transmission lines and transformers to distribute electricity to homes and industries around each state. Voltages can be a ...
10.1 Properties of Electric Charges
10.1 Properties of Electric Charges

Electromagnetic Waves Electromagnetic Waves
Electromagnetic Waves Electromagnetic Waves

... • Suppose an unpolarized light beam is incident on the first on a polarizing sheet (called polarizer). The light that is passing through is polarized vertically. Its intensity is reduced to half its original value. • A 2nd polarizing sheet (called analyzer) intercepts this beam with its transmission ...
Metals that are magnetic
Metals that are magnetic

... 1. All magnets are surrounded by an invisible force called the ________________ _______________ 2. The north pole of one magnet will be attracted to the ______ pole of another magnet. 3. The poles of the earth can move. True or False? 4. In the far north, radiation from the sun is reflected off the ...
Chapter 28 Sources of the magnetic field
Chapter 28 Sources of the magnetic field

Gauss` Law and Applications
Gauss` Law and Applications

11. Ultralow  Temperature  Studies  of Electronic Layers
11. Ultralow Temperature Studies of Electronic Layers

... magnetoresistance of our MOSFET's at ultralow temperatures. magnetoresistance oscillations similar to those seen previously in ultranarrow metal wires and narrow strips of GaAs. The magnitude of the magnetoresistance fluctuations is about the same as that of the fluctuations of resistance with gate ...
PHYS 272 Fall 2007 Monday, December 10, 2007 Final Exam - A
PHYS 272 Fall 2007 Monday, December 10, 2007 Final Exam - A

... The magnetic field is uniform and out of the page inside a circle of radius R. The magnetic field is essentially zero outside the circular region. The magnitude of the field as a function of time is (B0 + bt 3 ). B0 and b are positive constants and t = time. What is the magnitude of the induced elec ...
Magnetism - Electrical and Computer Engineering Department
Magnetism - Electrical and Computer Engineering Department

... Hysteresis Loop • Some ferrites, have almost rectangular B-H curves, ideal for digital computers for storing information. • The area of the loop gives the energy loss per volume during one cycle in the form of heat. • Tall-narrow loops are desirable for electric ...
Magnetic Fields
Magnetic Fields

A neutrally charged object has equal numbers of electrons and
A neutrally charged object has equal numbers of electrons and

... When an object becomes charged it either: gains electrons  becomes negatively charged.  loses electrons  becomes positively charged. NB electrons that are orbiting the nucleus of an atom are easily removed or accepted where protons that are tightly bound up in the nucleus are not. Electrons are ...
Chapter TM27
Chapter TM27

exam2
exam2

Name . E field Voltage prac
Name . E field Voltage prac

< 1 ... 547 548 549 550 551 552 553 554 555 ... 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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