Superdiamagnetism

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superconductor
acts as an essentially perfect diamagnetic material when placed in a magnetic field and it excludes the field, and so the flux lines completely avoid the region

Superdiamagnetism (or perfect

magnetic permeability (i.e. a volume magnetic susceptibility
= −1) and the exclusion of the interior magnetic field.

Superdiamagnetism established that the superconductivity of a material was a stage of phase transition. Superconducting magnetic levitation is due to superdiamagnetism, which repels a permanent magnet which approaches the superconductor, and flux pinning, which prevents the magnet floating away.

Superdiamagnetism is a feature of superconductivity. It was identified in 1933, by Walther Meissner and Robert Ochsenfeld, but it is considered distinct from the Meissner effect which occurs when the superconductivity first forms, and involves the exclusion of magnetic fields that already penetrate the object.

Diagram of the Meissner effect. Magnetic field lines are excluded from a superconductor when it is below its critical temperature.

Theory

thermodynamic state would be described by a single wave function
.

"Screening currents" also appear in a situation wherein an initially normal, conducting metal is placed inside a magnetic field. As soon as the metal is cooled below the appropriate transition temperature, it becomes superconducting. This expulsion of magnetic field upon the cooling of the metal cannot be explained any longer by merely assuming

zero resistance and is called the Meissner effect. It shows that the superconducting state does not depend on the history of preparation, only upon the present values of temperature, pressure and magnetic field, and therefore is a true thermodynamic state
.

See also

References

  • Shachtman, Tom, Absolute Zero: And the Conquest of Cold. Houghton Mifflin Company, December 1999.