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Flux penetration into flat superconductors of arbitrary shape
Flux penetration into flat superconductors of arbitrary shape

... electric field and the exponent n is determined by the activation energy U. Namely, the often observed dependence U( j)5U c ln(jc /j) yields E( j)5E c exp(2U/kT)5Ec(j/jc)n with n5U c /kT. Using this model in Refs. 10 and 61 the current distribution was calculated for rectangular specimens and nice a ...
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... (B) It is unaffected because the frequency of the phase change is an integral multiple of . (C) It is destroyed except when the phase difference is 0 or . (D) It is destroyed for all phase differences because the monochromaticity of the sources is destroyed. (E) It is not destroyed but simply shif ...
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... lines escape). Since dA points outward, the dot product in the integral is positive for B-field pointing out and negative for B-field pointing in. There is also a corresponding differential form of this equation covered in Maxwell's equations below. Energy is needed to generate a magnetic field both ...
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... One factor limiting computer chip speeds is the waste heat they produce. The more computations per second a chip performs, the more heat it produces and the greater the danger of electronic failure. A chip is a collection of transistors and connecting wires. Functionally, a transistor is an on/off s ...
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Review Exam 4

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Quasi-one-dimensional spin nematic states and their excitations Oleg Starykh, University of Utah

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What Now??? - UCF Physics

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The difference of the magnetic fields created by currents in neutral

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dina maizana - UniMAP Portal

... Its magnetic force clockwise when observed from the right. This direction of spin may be term positive. If the electron caused to turn over, it will appear to spin in the opposite or negative direction when observed from above, its magnetic force now counter-clockwise from the right. When an atomic ...
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Time Harmonic Fields

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Chapter 4: Magnetostatics

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Chapter #10 magnetism-multiple

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Superconductivity



Superconductivity is a phenomenon of exactly zero electrical resistance and expulsion of magnetic fields occurring in certain materials when cooled below a characteristic critical temperature. It was discovered by Dutch physicist Heike Kamerlingh Onnes on April 8, 1911 in Leiden. Like ferromagnetism and atomic spectral lines, superconductivity is a quantum mechanical phenomenon. It is characterized by the Meissner effect, the complete ejection of magnetic field lines from the interior of the superconductor as it transitions into the superconducting state. The occurrence of the Meissner effect indicates that superconductivity cannot be understood simply as the idealization of perfect conductivity in classical physics.The electrical resistivity of a metallic conductor decreases gradually as temperature is lowered. In ordinary conductors, such as copper or silver, this decrease is limited by impurities and other defects. Even near absolute zero, a real sample of a normal conductor shows some resistance. In a superconductor, the resistance drops abruptly to zero when the material is cooled below its critical temperature. An electric current flowing through a loop of superconducting wire can persist indefinitely with no power source.In 1986, it was discovered that some cuprate-perovskite ceramic materials have a critical temperature above 90 K (−183 °C). Such a high transition temperature is theoretically impossible for a conventional superconductor, leading the materials to be termed high-temperature superconductors. Liquid nitrogen boils at 77 K, and superconduction at higher temperatures than this facilitates many experiments and applications that are less practical at lower temperatures.
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