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Introduction to Electromagnetic Theory Electromagnetic radiation
Introduction to Electromagnetic Theory Electromagnetic radiation

III
III

Lecture 8 - McMaster Physics and Astronomy
Lecture 8 - McMaster Physics and Astronomy

... We then define electric potential difference dV by ...
Student understanding of forces on charges in magnetic fields Gordon J. Aubrecht, II,
Student understanding of forces on charges in magnetic fields Gordon J. Aubrecht, II,

... Cristian Raduta, Department of Physics, Ohio State University Although physics is the same worldwide, students belonging to different learning systems (or different cultural environments) may develop different styles of approaching and reasoning out physics problems. We compare student physics probl ...
Chapter 7 Magnetism: Electromagnets
Chapter 7 Magnetism: Electromagnets

Abstract
Abstract

A  B
A B

tutor 3
tutor 3

... 1. The same amount of charge is contained inside the Gaussian surface in each case so the E field is the same. 2. a and b contain all of the charge and so see the same E field. Less charge is contained in c and d and hence the E field is lower in c and lower yet in d. 3. The forces from opposing poi ...
PPT - LSU Physics
PPT - LSU Physics

... A Source of Magnetic Field • Orested’s Observation : an electric current creates a magnetic field • Simple experiment: hold a ...
Name: Practice – 19.2 Electric Potential in a Uniform Electric Field 1
Name: Practice – 19.2 Electric Potential in a Uniform Electric Field 1

Magnetic Field Outside an Ideal Solenoid—C.E. Mungan, Spring
Magnetic Field Outside an Ideal Solenoid—C.E. Mungan, Spring

Chern-Simons Theory of Fractional Quantum Hall Effect
Chern-Simons Theory of Fractional Quantum Hall Effect

Name
Name

Lecture 17
Lecture 17

... in any medium except vacuum depends on the wavelength of the light. The dependence of n on wavelength implies that when a light beam consists of rays of different wavelengths, the rays will be refracted at different angles by a surface; that is, the light will be spread out by the refraction. This s ...
practice exam
practice exam

... distributed over it. A point charge Q is placed at the center of the ring. The electric field is equal to zero at field point P, which is on the axis of the ring, and 0.73 m from its center. What is the value for the point charge Q? Show work. [Hint: V for a ring of charge is given above.] ...
Jeopardy
Jeopardy

... a loop of wire with a clockwise current as shown? Into the board inside the loop, out of the board outside the loop ...
An Old Final Exam - Linn-Benton Community College
An Old Final Exam - Linn-Benton Community College

... 13. An equipotential surface must be A) parallel to the electric field at any point. B) perpendicular to the electric field at any point. 14. One coulomb per volt is a A) watt. B) farad. C) electron-volt. D) joule. 15. Two 3.00-μC charges are at the ends of a meter stick. Find the electrical potent ...
Motion of charged particles in B *Code: 27L1A009, Total marks: 1
Motion of charged particles in B *Code: 27L1A009, Total marks: 1

G. Maxwell`s Equations: Integral Form
G. Maxwell`s Equations: Integral Form

... 1. We started with Coulomb's Law. The first equation is Gauss's Law, which is an alternate form of Coulomb's Law. 2. Then we used special relativity and Coulomb's Law to arrive at the magnetic field. The field lines closed on themselves for our line of current. Therefore, there are no net magnetic-f ...
Physics 12 Electric Potential Notes.
Physics 12 Electric Potential Notes.

Two-electron Interference
Two-electron Interference

... quantum interference of two independent, but indistinquishable, particles is also  possible. For a single particle, the interference is between the amplitudes of the particle’s  wave function, whereas the interference between two particles is a direct result of  quantum exchange statistics. Such int ...
Slide 1
Slide 1

Document
Document

... of a spatially uniform electric field. This electrokinetic phenomenon was observed for the first time in 1807 by Reuss, who noticed that the application of a constant electric field caused clay particles dispersed in water to migrate. It is ultimately caused by the presence of a charged interface be ...
Atomic and Molecular Physics for Physicists Ben-Gurion University of the Negev
Atomic and Molecular Physics for Physicists Ben-Gurion University of the Negev

... But, if we put a detector behind each slit, we find that the photon passes only through one of the slits each time! ...
February 8 Magnetism
February 8 Magnetism

< 1 ... 596 597 598 599 600 601 602 603 604 ... 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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