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Exam 3 Solutions
Exam 3 Solutions

Worksheet 6.5 - Equipotential Lines and Changes in Energy
Worksheet 6.5 - Equipotential Lines and Changes in Energy

Section 3.7
Section 3.7

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Practice Final Exam

Chapter 25 QQ
Chapter 25 QQ

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... 4. (15) Use cylindrical coordinates to calculate the divergence of a vector field u =(z x, 0, 0). Make sure the result agrees with the divergence calculated using Cartesian coordinates. Verify the divergence theorem for this field, with volume V equal to the part of the cylinder x2+y2≤4 lying in the ...
January 2002
January 2002

104 Phys Lecture 1 Dr. M A M El
104 Phys Lecture 1 Dr. M A M El

Magnetism and Electricity
Magnetism and Electricity

... magnetic poles, so the magnetic field points from north poles to south poles. The magnetic field may be represented by magnetic field lines. The closer together (that is, the denser) the B field lines, the stronger the magnetic field. At any location, the direction of the magnetic field is tangent t ...
9.3
9.3

Chapter 5 Question Set
Chapter 5 Question Set

... 14. Why do you think bending a wire does not affect its electrical resistance even though a bent pipe offers more resistance to the flow of water than a straight one? Answer: Because the charge and current flowing through a wire flows through the metal atoms themselves. The charge flows through the ...
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... current. This effect is called electromagnetic induction, because the changing magnetic field induces an electric field which can cause a current in a conductor. Such an induced current also produces a magnetic field whose net effect is to oppose the change that produced the current in the first pla ...
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Tue_10.00-Cadez

The Inner Magnetosphere
The Inner Magnetosphere

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Document

Millikan Experiment
Millikan Experiment

Electric Field - Purdue Physics
Electric Field - Purdue Physics

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Lecture 2

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1. This question is about forces on charged particles in electric and

... This question is about the force between current­carrying wires.  Diagram 1 below shows two long, parallel vertical wires each carrying equal currents in the  same direction. The wires pass through a horizontal sheet of card. Diagram 2 shows a plan view  of the wires looking down onto the card.  ...
In a television set, electrons are first accelerated from rest through a
In a television set, electrons are first accelerated from rest through a

The gauge non-invariance of Classical Electromagnetism
The gauge non-invariance of Classical Electromagnetism

1.  Assume a plane wave in vacuum for which... and the amplitude of the electric field is E 
1. Assume a plane wave in vacuum for which... and the amplitude of the electric field is E 

Physics 216 Spring 2012 Quantum Mechanics of a Charged Particle
Physics 216 Spring 2012 Quantum Mechanics of a Charged Particle

... the classical Hamiltonian of a charged particle in an electromagnetic field. We then use this result to obtain the Schrodinger equation using the principle of minimal substitution. We examine a special case of a uniform magnetic field. Finally, we demonstrate the origin of the coupling of the spin o ...
Lecture Notes, Feb 29
Lecture Notes, Feb 29

Electromagnetism - Sterling Public Schools
Electromagnetism - Sterling Public Schools

... The intensity or strength of an electric or magnetic field can be determined by the lines representing it. The field intensity is proportional to the number of lines of force per unit area normal to the field. High intensity is represented by lines drawn close together, low intensity is represented ...
< 1 ... 575 576 577 578 579 580 581 582 583 ... 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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