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Maxwell`s Equations in Differential Form
Maxwell`s Equations in Differential Form

Magnetization - Purdue Physics
Magnetization - Purdue Physics

GG 450 Lecture 13 Feb 8, 2006
GG 450 Lecture 13 Feb 8, 2006

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Lecture 8 ppt version

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Magnetic Field Simulation of an Induction Motor Using P. Pao-la-or

... circuit of induction motors. The test system previously described is simulated by an FEM solver written in C. The simulation are performed in a 1.6 GHz, 512-MB SD-RAM Pentium IV computer. Due to the steady-state operation, the simulated time step (∆t = 0.1145 ms for ∆θ = 1° of the rotor movement) is ...
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slides - 7th MATHEMATICAL PHYSICS MEETING
slides - 7th MATHEMATICAL PHYSICS MEETING

... At this stage, the Universe was in a quantum state, which should be described by a wave function (complex valued and depends on some real parameters). But, QC is related to Planck scale phenomena - it is natural to reconsider its foundations. We maintain here the standard point of view that the wave ...
Homework No. 05 (Fall 2013) PHYS 320: Electricity and Magnetism I
Homework No. 05 (Fall 2013) PHYS 320: Electricity and Magnetism I

2_03_Electrical and electronics engineering
2_03_Electrical and electronics engineering

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... Magnetic fields In physics, a field means a region where an object experiences a force without being touched. For example, there is a gravitational field around the Earth. This attracts mass towards the Earth’s centre. Magnets are surrounded by magnetic fields and electric charges by electric field ...
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Electromagnetic Theory

... µ0 q Ẋ ( t′ ) A ( t, x ) = --------- ---------------------------------------------------------------------------4π Ẋ ( t′ ) ⋅ ( x – X ( t′ ) ) x – X ( t′ ) – -------------------------------------------c µ0 q Ẋ ( t′ ) = ----------- ----------------------------------4πr′ [ 1 – β ( t′ ) ⋅ n′ ] Hence ...
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... 11. A person is standing in front of a diverging (convex) mirror. What type of image does the mirror form of the person? 1. erect, virtual, and smaller than the person 3. erect, real, and smaller than the person 2. erect, virtual, and the same size as the person 4. erect, real, and the same size as ...
Exam #: Printed Name: Signature: PHYSICS DEPARTMENT
Exam #: Printed Name: Signature: PHYSICS DEPARTMENT

... region occupied by the torus a distance r from the center. b) Under what conditions can the magnetic field inside the torus be considered to have approximately uniform magnitude? c) Argue that the magnetic field outside the torus is not zero. d) What is the direction of the magnetic field at the cen ...
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Physics 12

... b. How much force is required to make the 34 μC move as indicated above? 6. An alpha particle (4 x mass of a proton and twice its charge) is travelling at 2.4 x 106 m/s when it is 8.0 m away from a 7.6 x 10-5 C positive charge. What is the alpha particle’s distance of closest approach (how close can ...
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REVIEW OF WAVE MECHANICS

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Path integral Monte Carlo

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Chapter 10 Exercises 5. An electron always experiences a force in

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orbital quantum number

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Magnetism 1. Which of the following does not create a magnetic field?

... parallel to both the magnetic field and then electron's velocity. parallel to magnetic field and perpendicular to electron's velocity. ...
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1 - אתר מורי הפיזיקה

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The Electric Potential

< 1 ... 485 486 487 488 489 490 491 492 493 ... 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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