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Physics 202 MVF10:20 Spring 2008 (Ford) Name (printed) Name
Physics 202 MVF10:20 Spring 2008 (Ford) Name (printed) Name

Physics 228, Lecture 12 Thursday, March 3, 2005 Uncertainty
Physics 228, Lecture 12 Thursday, March 3, 2005 Uncertainty

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Electromagnetic Fields Lecture

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Single Particle Motion

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electric field

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Magnetic fields of stars and planets
Magnetic fields of stars and planets

SYLLABUS PHYSICS 208: Electricity, Magnetism
SYLLABUS PHYSICS 208: Electricity, Magnetism

8.4 Motion of Charged Particles in Magnetic Fields
8.4 Motion of Charged Particles in Magnetic Fields

... forces? We need a scientific model that describes different types of forces that exist at different points in space, and field theory does that. Field theory is a scientific model that describes forces in terms of entities, called fields, that exist at every point in space. The general idea of field ...
Electric fields are
Electric fields are

... Electric fields are force fields produced by electric charges. They can extend throughout space, and influence other charges (and currents and magnetic fields, as you will discover later in the course). Electric Field Lines graphically represent electric fields. They show you the direction and relat ...
E-field and Electric Potential Practice Problems
E-field and Electric Potential Practice Problems

Electric Potential Practice Problems
Electric Potential Practice Problems

Electric Field Hockey
Electric Field Hockey

The field produced by charges in a slab of finite thickness “d”
The field produced by charges in a slab of finite thickness “d”

1 - INFN Roma
1 - INFN Roma

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Title here

Towards a perturbative treatment of gravitational wave memory
Towards a perturbative treatment of gravitational wave memory

... memory: one due to angular distribution of energy radiated to null infinity, the other due to a change in the Err component of the Weyl tensor. • The effect is primarily due to the l =2 piece. ...
Electric Field Hockey
Electric Field Hockey

Magnetic fields lecture notes
Magnetic fields lecture notes

... A charged particle is moving perpendicular to a magnetic field in a circle with a radius r. An identical particle enters the field, with v perpendicular to B, but with a higher speed v than the first particle. Compared to the radius of the circle for the first particle, the radius of the circle for ...
Resonant tunnelling through a single level with non-collinear magnetizations
Resonant tunnelling through a single level with non-collinear magnetizations

Slides - Indico
Slides - Indico

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Basic concepts in quantum mechanics

... heavy (formally Mk = ∞) that they are treated as static particles. One key feature of all these Coulombic Hamiltonians is that the range of the Hamiltonian function H is the whole R, in particular arbitrarily negative energies can be achieved. Assuming some radiation mechanism that is able to suck e ...
< 1 ... 405 406 407 408 409 410 411 412 413 ... 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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