Reference Frames and Relative Motion Uniform Circular Motion
... Magnetic Fields We know about the existence of magnetic fields by their effect on moving charges. The magnetic field exerts a force on the moving charge. ...
... Magnetic Fields We know about the existence of magnetic fields by their effect on moving charges. The magnetic field exerts a force on the moving charge. ...
Brief Introduction to Superconductivity
... state of two electrons. Electrons repel each other in vacuum but under certain circumstances when in a crystal lattice they can attract each other and form a Cooper pair. Electrons have spins. Spin is a number (a quantum number) that characterizes the response of the electrons to a magnetic field an ...
... state of two electrons. Electrons repel each other in vacuum but under certain circumstances when in a crystal lattice they can attract each other and form a Cooper pair. Electrons have spins. Spin is a number (a quantum number) that characterizes the response of the electrons to a magnetic field an ...
The Wizard Test Maker
... x 10-2 meter from a second point charge of +4.0 x 10-7 coulomb. The magnitude of the electrostatic force between the charges is (A) 2.7 N ...
... x 10-2 meter from a second point charge of +4.0 x 10-7 coulomb. The magnitude of the electrostatic force between the charges is (A) 2.7 N ...
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.