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PPT
PPT

The Millikan Experiment: Determining the Elementary
The Millikan Experiment: Determining the Elementary

... • An electron is fired horizontally at 2.5 x 106 m/s between two horizontal parallel plates 7.5 cm long, as shown in Figure 7. The magnitude of the electric field is 130 N/C. The plate separation is great enough to allow the electron to escape. Edge effects and gravitation are negligible. Find the v ...
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Document

Homework 2
Homework 2

... Recall that the linear charge density is 1 C/m and the unit of length is 1m. Whenever there is a relationship between two physical quantities expressed in the form of an equation, the units on both sides must be the same. This requires that the coefficient α in the equation λ(x) = αx has unit C/m2. ...
30) Magnetic Mass Flow We will calculate the flow of mass in a
30) Magnetic Mass Flow We will calculate the flow of mass in a

Conservative forces
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L28.ppt - University of Iowa Physics

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... 2. Where do magnetic field lines begin? Where do they end? Explain. 3. An unmagnetized nail will not attract an unmagnetized paper clip. However, if one end of the nail is in contact with a magnet, the other end will attract a paper clip. Explain. 4. A student has placed two cylindrical permanent ma ...
2.  Derive  an  expression  for ... charges together as indicated in Fig. 28-28 below. Each side... Homework #4     203-1-1721   ...
2. Derive an expression for ... charges together as indicated in Fig. 28-28 below. Each side... Homework #4 203-1-1721 ...

... 4. The electric field inside a nonconducting sphere of radius R, containing a uniform charge density, is radially directed and has magnitude E = (qr)/(4 oR3), where q is the total charge in the sphere and r is the distance form the center of the sphere. (a) Find the potential V inside the sphere, ta ...
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Chapter 5.3 Q1 The positive charge on the rod will attract electrons

... E1 = 21 = 4! k" 1 = 4! $ 8.99 $109 $ 6.4 $10#6 = 7.2 $105 N C#1 and r1 E2 = 4! k" 2 = 4! $ 8.99 $109 $ 4.2 $105 = 4.8 $105 N C#1 . (d) The electric field is largest for the sphere with the larger charge density. The wire has to be long so that the charge of one sphere will not affect the charge dist ...
PHYS 102 Problems - Chapter 20 – Set 8 Feb. 2, 2010
PHYS 102 Problems - Chapter 20 – Set 8 Feb. 2, 2010

... Alpha particles of charge q = +2e and mass m = 6.6 x 10-27 kg are emitted from a radioactive source at a speed of 1.6 x 107 m/s. What magnitude field strength would be required to bend them into a circular path of radius r = 0.25 m? In this scenario, the magnetic force is causing centripetal motion, ...
Magnetism and Matter
Magnetism and Matter

< 1 ... 616 617 618 619 620 621 622 623 624 ... 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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