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7. Capacitance
7. Capacitance

Powerpoint
Powerpoint

... which would have the greater acceleration? Which has the greater potential energy when released? Which will have a greater speed when at the bottom of the hill? 4. What factors does the speed at the bottom of the hill depend on? What factors does the acceleration of the ball depend on? 5. Is it poss ...
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Fundamental Properties of Superconductors - Wiley-VCH

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Electric Potential Practice Problems

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THE MALAY COLLEGE KUALA KANGSAR INDIVIDUAL

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... With sufficient external current, this effect can locally drive the current density to zero or even negative. This situation can persist for many seconds in hot JET plasmas due to the long current diffusion time. This effect can be seen in a simulation of the evolution of the flux surface averaged c ...
Electromagnetism and Relativity
Electromagnetism and Relativity

Sheath properties nd related phenomena of the plasma wall
Sheath properties nd related phenomena of the plasma wall

... The experiments were performed on Pilot-PSI linear device, during our team-members mobility at FOM Institute for Plasma Physics “Rijnhuizen”, The Netherlands. Milestone 1: Katsumata probe measurements for diffusion coefficient The Katsumata probe was inserted in Pilot PSI device at about 2 cm in fro ...
Particle Accelerators for High Energy Physics A Short History
Particle Accelerators for High Energy Physics A Short History

230/ch30 Biot-Savart Ampere
230/ch30 Biot-Savart Ampere

... the point r = x, y, z where we calculate the magnetic field. ur =   r − r1 It is often useful to give the charges dQ and their velocity the index 1, as a reminder that the location of the current segment (the charge density, the charge etc) is different from the location where we calculate the mag ...
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PDF Transparencies

Which Statement best describes why tiny bits of paper are attracted
Which Statement best describes why tiny bits of paper are attracted

Lecture 2 - Department of Applied Physics
Lecture 2 - Department of Applied Physics

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Slide 1

...  If WAB is +ve, then B is at a higher potential than A.  Units are work/charge = joule/coulomb ≡ volt (V).  Potential difference is a scalar quantity  Potential energy refers to a charge-field system (work done to introduce a charge to a field). Electric potential is a scalar characteristic of a ...
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Manuscript: Trapped-ion quantum logic with global radiation fields
Manuscript: Trapped-ion quantum logic with global radiation fields

Planar Cell PDF
Planar Cell PDF

... charged groups on the material surface will lead to the attraction of buffer salts to the surface. The closest salts will be strongly attracted forming the Stern layer at the surface of the material under study. Further from the surface, buffer salts will be attracted to the material but will not be ...
Quantum motion of electrons in topologically distorted crystals
Quantum motion of electrons in topologically distorted crystals

From photoelectric effect to digital imaging
From photoelectric effect to digital imaging

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CERN and Bubbel Chamber Detective
CERN and Bubbel Chamber Detective

... following rules will allow you to analyze photographs of such events from a bubble chamber at CERN in Switzerland, the home of the Large Hadron Collider.  Centripetal acceleration a = v2/r. The force of a magnetic field on a charged particle is given by F = qvB = m v2/r. Therefore the momentum of t ...
Fine structure constant and square root of Planck momentum
Fine structure constant and square root of Planck momentum

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2005

... temperature [4]. Bragg diffraction was used to create two spatially separated wave packets, which would interfere during expansion, analogous to a Young’s double slit experiment. Fringe visibility greater than 90% was observed in a thermal cloud. We have shown that interference is lost when the sep ...
Notes - Electrostatics
Notes - Electrostatics

... In conductors excess electrons will move  when an electric field is present. For “steady state” (i.e. no moving charges), the net electric field must be zero. ...
R.H. Austin, N. Darnton, R. Huang, J.C. Sturm, O. Bakajin, and T. Duke, "Ratchets: the problem with boundary conditions in insulating fluids," Appl. Phys. A 75, pp. 279-284 (2002).
R.H. Austin, N. Darnton, R. Huang, J.C. Sturm, O. Bakajin, and T. Duke, "Ratchets: the problem with boundary conditions in insulating fluids," Appl. Phys. A 75, pp. 279-284 (2002).

... (so that i = −i and ∇ i = −∇ −i then φi = −φ−i and the distribution broadens, but the mean cannot shift. There is no asymmetric flux. Does this mean these devices cannot work? No, they can work in two ways. First, if the force lines actually penetrate the obstacles rather than pass around them the ...
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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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