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How current loops and solenoids curve space-time
How current loops and solenoids curve space-time

grain charging in weakly ionized plasma in the presence of external
grain charging in weakly ionized plasma in the presence of external

expansion and diffusion of a laser plasma in a magnetic field
expansion and diffusion of a laser plasma in a magnetic field

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Electromagnetic Waves in Media with Ferromagnetic Losses

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... one volt creates one electron volt - it just basically simplifies the math involved). Equipotential Diagrams - analogous to a topographic map - showing lines of equal potential (V) just as a topographic map shows contours of equal height. When you walk on a contour line, your potential energy stays ...
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Non-isolated Constant Current Linear LED Driver BL8312

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Particle Accelerators for High Energy Physics A Short History

... reasonable approximation to a dipole magnet for our purposes here. A similar matrix applies in the other transverse degree of freedom, with reversal of lens focusing character. Stability requires that M n remain finite for arbitrarily large n, and an eigenvalue analysis quickly shows that this will ...
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Experimental Study on the Mössbauer Effect of ⁵⁷Fe in

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Ch.42- p-n junctions, LED, solar cell, MOSFETs and superconductivity

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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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