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14 - Basic Theory of Nuclear Magnetic Resonance
14 - Basic Theory of Nuclear Magnetic Resonance

... photon (or 3.99x10-13 kJsmol-1). Since the usual strength of a chemical bond is about 400 kJmol-1, electromagnetic wave energies above the visible region in Table 1 have more than enough energy to photodissociate (break) chemical bonds, while waves below the visible region cannot typically break mol ...
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... a. Calculate the induced emf in the loop. b. Indicate the direction of the induced current. c. Calculate the induced current in the loop. d. Calculate the rate of thermal energy that is produced in the loop. 2. A simple generator has a square armature with 1000 loops that are 15 cm on a side. The ar ...
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... The Chemical Shift of Different Protons NMR would not be very valuable if all protons absorbed at the same frequency. You’d see a signal that indicates the presence of hydrogens in your sample, but any fool knows there’s hydrogen in organic molecules. What makes it useful is that different protons ...
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ideas to implimentation notes File

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Dirac`s Conception of the Magnetic Monopole, and its Modern Avatars

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NMR Spectroscopy: Principles and Applications

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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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