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Electric Field
Electric Field

Electric Field
Electric Field

What are electromagnetic waves?
What are electromagnetic waves?

... Intensity of electromagnetic waves A nyodenium-glass laser emits short pulses of high-intensity electromagnetic waves. The electric field has an rms value of 2.0 × 109 N/C. Find the average power of each pulse that passes through a 1.6 × 10−5 − m2 surface that is perpendicular to the laser beam. ...
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The Sun

... within the Sun. – The waves stand between various boundaries – The boundaries are created by the temperature dependence of the velocity of sound. – As a wave travels down it is reflected by the continuous variation in sound speed. It can only penetrate to a given depth. As it returns it is reflected ...
of THE by 0.
of THE by 0.

... reabsorption) that is regarded as the mechanism by which the electron interacts with the zero-point field. It must be emphasized that this mechanism of photon emission and absorption is a very convenient way of handling radiation problems. ...
Syllabus - Department of Electrical Engineering
Syllabus - Department of Electrical Engineering

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important derivations type questions

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... A charged object (the rod) is placed in contact with another object (the sphere) Some electrons on the rod can move to the sphere When the rod is removed, the sphere is left with a charge The object being charged is always left with a charge having the same sign as the object doing the charging ...
Problem Set 3
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Honors Physics Electric Potential Energy and Potential Difference

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PHYS 272 Fall 2010 Practice Exam 1

... There are two parts to the Exam 1, part 1 is a machine-graded test (multiple choice problems) and part 2 is a separate test that you turn in to be graded by hand. A formula sheet is provided (see end page). Machine Answer Sheet: Using a pencil, fill in Last Name, First Name, & Middle Initial, plus y ...
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... The magnitude of the force on the wire is found by F  ILB sin   20 A0.10 m0.8T sin 45  1.13 N The direction of the force can be found by the right-hand rule. Place your fingers in the direction of the magnetic field, and your thumb in the direction of the length (and current) which is per ...
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Chapter 30 - Sources of Magnetic Fields

... classical description) and this motion constitutes charge traveling around a circular path. Therefore, there is a magnetic moment associated with the spin. ...
Chapter 30 - Sources of Magnetic Fields
Chapter 30 - Sources of Magnetic Fields

LAWS, RULES, PRINCIPLES, EFFECTS, PARADOXES, LIMITS,
LAWS, RULES, PRINCIPLES, EFFECTS, PARADOXES, LIMITS,

... The EPR effect demonstrates that if one of the particles isdetected, and its spin is then measured, then the other particle-- no matter where it is in the Universe -- instantaneously isforced to choose as well and take on the role of the otherparticle. This illustrates that certain kinds of quantumi ...
< 1 ... 388 389 390 391 392 393 394 395 396 ... 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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