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L6 Lorentz force
L6 Lorentz force

... The relation between the magnetic field B and the magnetic force FB on a point charge q is more complicated: FB = q v×B , where v is the velocity of the moving charge. • The force is proportional to q, including the sign of q. • The force is proportional to B. • The force is proportional to v. • Whe ...
KEY - AP Physics– Electrostatics – FR 1 #1 (1975
KEY - AP Physics– Electrostatics – FR 1 #1 (1975

Notes on MHD - MSU Solar Physics
Notes on MHD - MSU Solar Physics

... Equation (4) is formally very similar to the equation for a trajectory (2), but with B/ρ taking the place of v and s taking the place of t. Like the trajectory (4) can be solved uniquely beginning at any point in space r(0) = r0 as an “initial condition”. This shows that there is a unique field line ...
1 PHYS 272 Fall 2010 Practice Exam 1 There are
1 PHYS 272 Fall 2010 Practice Exam 1 There are

PHYS 308
PHYS 308

Lecture
Lecture

Physics 2018: Great Ideas in Science: The Physics Module Quantum
Physics 2018: Great Ideas in Science: The Physics Module Quantum

Notes On Plane Electromagnetic Waves
Notes On Plane Electromagnetic Waves

... the "foot" of our electric field line, which was initially at y = 0 at t = 0 , will be a distance -VT down the y-axis at time t = T. However, we have assumed that the information that this field line is being dragged downward can only propagate outward from x = 0 with the speed of light, c. Thus the ...
Antennas
Antennas

Electric Field - Purdue Physics
Electric Field - Purdue Physics

... • If the electric potential is a property of the field, how do we calculate it? • The electric potential of a field at a point @1 is the work per unit charge required to move from the reference point, @1A , , to the point, @1: ...
Electric Field - Purdue Physics
Electric Field - Purdue Physics

Class 20
Class 20

... However, there are some forces for which work does not depend on the path taken between the beginning and ending points. These are called conservative forces. A mathematically equivalent way to put this is that the work done by a conservative force along any closed path is exactly zero. ...
New Experimental Test of Coulomb`s Law: A - Exvacuo
New Experimental Test of Coulomb`s Law: A - Exvacuo

Magnetic Field and Electric Current I
Magnetic Field and Electric Current I

... Since external magnetic field affects motion of the charged particles, it should also affect the current-carrying wire, because electric current consists of moving electric charges. We saw how electric charges inside of the wire were shifted by external magnetic field. Positive charges are shifted t ...
Ch. 19 Magnetic fields
Ch. 19 Magnetic fields

... X X X X X X X X X X X X X X ...
SR Theory of Electrodynamics for Relative Moving Charges
SR Theory of Electrodynamics for Relative Moving Charges

Document
Document

... only qualitatively because the additional attraction of the electron back to the plate is not included  Due to surface imperfections, the surface field changes and can make large difference in the results ...
Electric Potential Difference
Electric Potential Difference

Lecture 4
Lecture 4

Force on a Current-Carrying Wire in a Magnetic Field F = ILB
Force on a Current-Carrying Wire in a Magnetic Field F = ILB

Field-Induced Gap in a Quantum Spin
Field-Induced Gap in a Quantum Spin

chapter 33 electric field
chapter 33 electric field

The Semiclassical Electron in a Magnetic Field and Lattice. Some
The Semiclassical Electron in a Magnetic Field and Lattice. Some

3 SUPERCONDUCTIVITY
3 SUPERCONDUCTIVITY

Relativistic Dynamics Dennis V. Perepelitsa
Relativistic Dynamics Dennis V. Perepelitsa

... For a dozen values of the magnetic field B that ranged from 65 to 125 Gauss, we recorded a two-minute energy spectra for multiple values of V , being careful to take at least six measurement of V in the vicinity of the value V0 that seemed to cause the maximum number of counts. Our step size was .15 ...
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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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