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Electricity and magnetism
Electricity and magnetism

... two point charges of different type: on a line through the charges, the field is from the positive to the negative between them, away from the positive and into the negative on the far side of them. In other regions, the field lines are bent curves since at any point it is the resultant of a vector ...
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File

ppt
ppt

File
File

FUTA-PDS Lecture notes
FUTA-PDS Lecture notes

Chap 14.
Chap 14.

Physics 272
Physics 272

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Adobe Acrobat file () - Wayne State University Physics and

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E/M writeup

Fields - Cathkin High School
Fields - Cathkin High School

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5. Fields and Electrical Physics

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r - PolyU EIE

to - Kendriya Vidyalaya Sector 8
to - Kendriya Vidyalaya Sector 8

... intensity at a point due to (i)an infinitely long uniformly charged straight wire (ii) a uniformly charged infinite sheet (iii) a uniformly charged thin spherical shell at an (a) outside point (b) inside point. Q3. (a)Deduce an expression for the capacitance of a parallel plate capacitor with air as ...
Homopolar Motor
Homopolar Motor

... This  can  be  done  by  using  a  second  rare-­‐earth  magnet,  and  making  sure  the   batteries  are  smaller  diameter  than  the  magnet  (or  using  washers  as  wheels).       ...
Arbitrary shaped wire I 均匀磁场中任意曲线导体
Arbitrary shaped wire I 均匀磁场中任意曲线导体

... 1) The directions of two fields. The E field due to a charge element is radial, whereas the M field due to a current element obeys right-hand rule. 2) The sources of two fields. An E field can be a result either of a single charge or a charge distribution, but a M field can only be a result of a cur ...
PRS_W15D2
PRS_W15D2

Physics 111 Fall 2007 Electrostatic Forces and the Electric Field
Physics 111 Fall 2007 Electrostatic Forces and the Electric Field

... 10. Four equal positive point charges, each of charge 8.0 µC, are at the corners of a square of side 9.2 cm. What charge should be placed at the center of the square so that all charges are at equilibrium? Is this a stable or unstable equilibrium in the plane? A negative charge must be placed at th ...
the Schrodinger wave equation
the Schrodinger wave equation

Chapter 4: Electric Potential
Chapter 4: Electric Potential

... In words, the work done by the conservative force moving the object from A to B equals the object’s initial potential energy minus the final potential B B energy. At the surface of the earth, the gravitational field points downward (the direction the gravitational force acts on objects). Suppose an ...
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Introduction to Electric Fields

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slides

Batteries don`t store charge. They store energy. A chemical battery
Batteries don`t store charge. They store energy. A chemical battery

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Exam 1 Solutions
Exam 1 Solutions

... FCoul q-Q = -kq|Q|/L2 is the Coulomb force to the left between +q and Q (the positive +q attracts the negative Q to the left, and the sign in front takes care of this direction) FCoul 3q-Q = +k(3q)|Q|/(d-L)2 is the Coulomb force to the right between Q and +3q (the positive +3q attracts the negative ...
AP Physics C Exam Questions 1991
AP Physics C Exam Questions 1991

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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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