What are aharonov bohm oscillations?
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It's a quantum mechanic effect.\n\nLike the electric Field E has a potential Phi, magnetic fields B have a vector potential A. When the quantum mechanic wave function (which describes matter, for example electrons, in quantum mechanics) travels through a vector potential A it picks up a phase shift, which can be demonstrated in an interference experiment, where the wave function is superposed with itself, by going two different ways. The funny thing is that one would expect that the magnetic field is the "physical relevant" quantity. But these interference pattern (the Aharonv-Bohm oscillations) also appear if both paths of the wave function are through field free space, it's just the vector potential that causes that effect.\n\nPhysicists were confused by that in the beginning, because neither the phase of a wave function can be observed, nor is the vector potential A uniq defined. You can do a so called gauge transformation, which changes the vector potential, but should leave all physical relevant quantities unchanged.\n\nThe solution to that puzzle is that you just measure phase differences in the interference experiment, not the pase itself. And the phase difference is gauge invariant.\n\nIf you don't understand everything: Don't worry, that's a popular question in a physics master exam!\n\nFor more information see the link below.
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If you have access to the Journal of Applied Physics, this should help:\nhttp://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=JAPIAU000076000009005380000001&idtype=cvips&gifs=yes
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A good starting point is wikipedia:\nhttp://en.wikipedia.org/wiki/Free-electron_theory_of_metals\n\nWhen you read this link, follow some of the referenced links for details on the specific applications you listed...\n\nHope this helps!
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Look up the mecahnical univers 43? on magnetic induction.
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Try,\n\nhttp://www.personal.psu.edu/faculty/d/x/dxh40/MBLemma.pdf
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http://en.wikibooks.org/wiki/Modern_Physics:Waves_in_one_Dimension:Problems
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Hi, \n\nThat's too much like real work, but think about it like breaking pool balls in classical, and wave interference with quantum. \n\nHope that helps, \nMatt
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Pauli thru his exclusion principle. For Bosons this is not absolutely true.
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i dont know much about physics but i did a search and this is what i got hope it has what you're looking for:\n\nhttp://science.electronicsinfoline.com/Physics/Electricity_and_Magnetism/
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http://hyperphysics.phy-astr.gsu.edu/Hbase/surten.html
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Use Kirchoff's laws.  Read page at link then follow the link "example."\n\nhttp://www.pa.msu.edu/courses/1997spring/PHY232/lectures/kirchoff/kirchoff.html\n\n--- \nadded:\nwow! pjw, that UTex link is a cool online tutorial!
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http://www.sitefoundry.com/biorhythms/
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Physics for Scientists and Engineers: extended version, Fifth Edition, Tipler & Mosca (Freeman. 2003).\n\nhttp://www.phy.cam.ac.uk/teaching/1A_2004-2005.pdf\n\nBAD KARMA,!!   WTF  Learn to spell douche!!\n\n:> peace
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Natural magnetic variations and decay.  It is like waves of variation.
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This is a relativistic problem The answer depents on the viewpoint of the observer. oscillation is a factor of time-mass-energy all of which are distorted relativisticaly. you are probably looking at an inverse square solution.\n\nContrary to popular belief electrons do not travel at relativistic velocities only their electromagnetic wave. This problem is further out there than you think.
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See if this helps.\n\nhttp://hyperphysics.phy-astr.gsu.edu/hbase/atomic/hund.html
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Mathematical method of quantum phase space is very useful in physical applications like quantum optics and non-relativistic quantum mechanics. However, attempts to generalize it for the relativistic case lead to some difficulties. One of problems is band structure of energy spectrum for a relativistic particle. This corresponds to an internal degree of freedom, so-called charge variable. In physical problems we often deal with such of dynamical variables that do not depend on this degree of freedom. These are position, momentum, and any combination of them. Restricting our consideration to this kind of observables we propose the relativistic Weyl--Wigner--Moyal formalism that contains some surprising differences from its non-relativistic counterpart