Superconductor

material capable of superconduction

A superconductor is a substance that conducts electricity without resistance when it becomes colder than a "critical temperature." At this temperature, electrons can move freely through the material. Superconductors are different from ordinary conductors, such as copper. Ordinary conductors lose their resistance (get more conductive) slowly as they get colder. In contrast, superconductors lose their resistance all at once. This is an example of a phase transition. High magnetic fields destroy superconductivity and restore the normal conducting state. Some examples of superconductors are the metals mercury and lead, ceramics and organic carbon nanotubes.

A magnet levitating above a high-temperature superconductor, cooled with liquid nitrogen. Persistent electric current flows on the surface of the superconductor. This excludes the magnetic field of the magnet (Faraday's law of induction). In effect, the current forms an electromagnet that repels the magnet

Normally, a magnet moving by a conductor produces currents in the conductor by electromagnetic induction. But a superconductor actually pushes out magnetic fields entirely by inducing surface currents. Instead of letting the magnetic field pass through, the superconductor acts like a magnet pointing the opposite way, which repels the real magnet. This is called the Meissner effect, and it can be demonstrated by levitating a superconductor over magnets or vice versa.

Explanation

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Physicists explain superconductivity by describing what happens when temperatures get cold. The thermal energy in a solid or liquid shakes the atoms so they randomly vibrate, but this gets less as the temperature drops. Electrons carry the same negative electric charge which makes them repel each other. At higher temperatures each electron behaves as if it were a free particle. There is also however a very weak attraction between electrons when they are in a solid or liquid. At rather large distances ( many hundreds of nanometers apart) and low temperatures (near absolute zero), the attractive effect and lack of thermal energy allows pairs of electrons to hang together. This is called a cooper pair and it is a quasiparticle, that is it acts as if it were a new kind of particle in its own right even though it is made up of two fundamental electrons.

Many overlapping cooper pairs can exist in the same nanometer sized space. Since paired electrons constitute a boson the motions of all of the cooper pairs within a single superconductor synchronize and they function as if they are a single entity. Small disturbances such as scattering of electrons are forbidden in this state, and it moves as one, showing no resistance to its motion. Thus, it is now a superconductor.

History of superconductors

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1911 superconductivity discovered by Heike Kamerlingh Onnes
1933 the Meissner effect discovered by Walter Meissner and Robert Ochsenfeld
1957 theoretical explanation for superconductivity put forward by John Bardeen, Leon Cooper, and John Schrieffer (BCS theory)
1962 the tunneling of superconducting Cooper pairs through insulating barrier predicted
1986 A ceramic superconductor was discovered by Alex Müller and Georg Bednorz. Ceramics are normally insulators. A lanthanum, barium, copper and oxygen compound with a critical temperature of 30K. Opened up the possibilities for new superconductors.
2020 Superconductor discovered that functions at room temperature[1]

Applications

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  • Superconducting quantum interference device (SQUID)
  • Powerful magnets
    • Particle accelerators
    • Small particle accelerators in health
    • Levitating trains
    • Nuclear fusion
    • MRI Scanner

References

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  1. ServiceOct. 14, Robert F.; 2020; Am, 11:00 (2020-10-14). "After decades, room temperature superconductivity achieved". Science | AAAS. Retrieved 2020-10-16. {{cite web}}: |last2= has numeric name (help)CS1 maint: numeric names: authors list (link)
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