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Fourier-based magnetic induction tomography for mapping resistivity
Fourier-based magnetic induction tomography for mapping resistivity

... where F is a filter threshold; k is the spatial frequency with k = 冑k2x + k2y where kx = p⌬k and ky = q⌬k 共p and q are integers兲; ⌬k = 2␲L / W 共W is the number of points along the x-axis in the W ⫻ W discrete mesh兲; S is the signal in k-space before filtering and S⬘ is the signal in k-space after fi ...
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... The resulting EDM has been criticized for being proportional to and nonvanishing as ma -> 0. The same issue arises in the case of the anomaly. The result is intrinsically oscillatory (the nonlocal makes the source for the vector potential transverse, ie, not Coulombic) . The above Feynman amplitudes ...
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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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