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Electromagnetic Induction (2) Electromagnetic Induction (1) Motional EMF ●
Electromagnetic Induction (2) Electromagnetic Induction (1) Motional EMF ●

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Superconductivity

... temperature to determine T c . You will use the thermocouple to measure the temperature, as above, and use a four point probe to measure the resistance. When a simple measurement of the resistance of an electrical test sample is performed by attaching two wires to it, the resistance of the wire-to-s ...
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... Current can be made to flow in a stationary wire by moving a magnetic field parallel  to the wire. _________________________________________________ The electromotive force depends only on magnetic field strength, the length of wire in the magnetic field, and the velocity  of the  wire in the magnet ...
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... and P2, shown in the figure below. The electron then passes through a small opening into a magnetic field of uniform field strength, B. As indicated, the magnetic field is directed into the page. The beam is stabilized and focused into a horizontal line by passing through charged plates P3 and P4. T ...
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CLASS-10TH -CHAPTER -13 MAGNETIC EFFECTS OF ELECTRIC CURRENT

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Ch. 19: CQ 4, 18, Pr. 9, 11, 15, 17, 28, 31, 39, 41, 43, 89
Ch. 19: CQ 4, 18, Pr. 9, 11, 15, 17, 28, 31, 39, 41, 43, 89

< 1 ... 516 517 518 519 520 521 522 523 524 ... 528 >

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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