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An Introduction to Kinetic Inductance Detectors

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... maximum? R = 1kΩ, C = 1 μfarad I V(t) ...
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... conductive wire can also increase the strength of the electromagnet. Changing the wire is one just way to change an electromagnets strength. Another way to change the strength is to change the other part of the electromagnet: the magnetic core. Some magnets are naturally stronger than others, so usi ...
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... The magnetic field is calculated using the MCD-method proposed by Gerth and Glagolevskij (2000, 2001). Nevertheless, this is not the only possible way. Calculations of the magnetic surface field can also be performed by other methods, such as described by Bagnulo et al. (1996) - using spherical harm ...
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... relatively cold. This difference in temperature is utilized to produce electrical energy. The warm surface water is used to boil a volatile liquid like ammoia. The vapours of the liquid are then used to run the turbine of generator and electricity is produced. 11. H=I2 RT = 25 x 20 x 30 H = 15000 J ...
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Kerr effect at high electric field in the isotropic

... One possibility is to add a term proportional to SE 4 with a fourth-order electric field to the Landau–de Gennes expansion. Introduction of such a term would produce dependences E 2 /δneff vs T − TNI that have a different tilt but the same intersection with the temperature axis for different values ...
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Conceptests II

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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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