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Electrical Characterization of Gold-DNA
Electrical Characterization of Gold-DNA

PHYSICS 241/261 EXAM I June 28, 2002
PHYSICS 241/261 EXAM I June 28, 2002

... This is a closed book exam. Print and encode your name, student ID number, and recitation number on the answer sheet. Answers to all questions are to be recorded on the answer sheet. There are 12 multiple-choice problems for a total of 100 points. Do not do the problems in the order in which they ar ...
Observation of Locally Negative Velocity of the Electromagnetic
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... calculus shows that the first (leftmost in time) maximum of the current will happen at tinter ¼ =ð2!c Þ. The time derivative of the current has its first maximum at tfar ¼ 0, and the first maximum of the current’s time integral is at tnear ¼ =!c . Hence, for the relative positions of the first max ...
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ppt - UCSB Physics

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Practice Packet for Chapter 16: Electric Forces and Fields (Due

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... field is of the order of the field of the pumping electromagnetic wave E0 ' 1V /m. That is believed to be very natural. Far from the reflecting region, below the wave amplitude maximum on the distance of several d, the largest ponderomotive force is fe3 (4) because it is inversely proportional to th ...
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... These formulas are for calculating the electric field at a location in space when you know the electric potential already and it is very easy to take its derivatives (parallel plates). It is better to use the point charge formulas for situations where point charges create the electric field and elec ...
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... Let rot be the frequency of rotations (Cycles/second) The velocity of particle v=2πrrot= r ωrot where ωrot=2πrot has units of radians/second and is called the angular velocity. The kinetic energy of the revolving particle is: ...
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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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