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Apparatus for Magnetization and Efficient Demagnetization of Soft
Apparatus for Magnetization and Efficient Demagnetization of Soft

the electromagnetic wave
the electromagnetic wave

Time, what is it? Dynamical Properties of Time
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... scale λJ [see Eq. (8)]. Instead, we find a saturation phenomenon for the diamagnetic moment at a field Bc [see Eq. (15)] controlled by the properties [Eqs. (9) and (10)] of the phase-polarized domains, i.e., the disorder pinning of the applied flux. This is followed by a depinning of the polarized d ...
The strange (hi)story of particles and waves
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Edge-mode superconductivity in a two
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... middle channel to be within 10% of the device centre. It is improbable that such an effect would occur in two separate devices from different growth batches and different superconductors, although we cannot exclude this possibility. The scenario above considers the possibility that interference path ...
Nonequilibrium transport in mesoscopic multi-terminal SNS Josephson junctions * M. S. Crosser,
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AP Physics B/C
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... L. The other end is attached to negatively charged wall. The electric field E due to the charged wall is constant in the vicinity of the charged sphere. The string makes a constant angle ϴ with the vertical. What is the sign and magnitude of charge q? ...
Russian Academy of Science Correspondence[1]
Russian Academy of Science Correspondence[1]

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... breakdown voltage VB, large currents start to flow. If there is no current limiting resistor which is connected in series to the diode, the diode will be destroyed. There are two physical effects which cause this breakdown. ...
CHAPTER 3: ELECTROMAGNETISM
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Modelling the solar wind interaction with Mercury by a quasi
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Full Text PDF

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Chapter 1 The Electric Force
Chapter 1 The Electric Force

... Representative electric field lines for the field due to a single positive point charge are shown in Figure 8 a. The electric field lines representing the field due to a single negative point charge are directed toward the charge (Fig.8 b). In either case, the lines are along the radial direction an ...
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Dynamical generation of wormholes with charged fluids in quadratic Palatini gravity
Dynamical generation of wormholes with charged fluids in quadratic Palatini gravity

... true meaning of curvature divergences in our theory since their existence seems to pose no obstacle for the wormhole extension. Let us note that these wormhole solutions correspond to static solutions of the field equations. Here we shall see that such solutions can be dynamically generated by probi ...
Wave nature of light
Wave nature of light

... Use the formula work = Force x Distance, along with uvast equations, Newton’s Laws and PCM in appropriate calculations Identify energy as the ability to do work Describe the different forms of energy State the principle of conservation of energy Be able to give examples of energy changes from one fo ...
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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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