Tractatus Logico-Philosophicus (6.5): Difference between revisions
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[[File:Superconductor.GIF|thumb|right|A [[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 [[diamagnetism]]''') is a [[phenomenon]] occurring in certain materials at [[low temperature]]s, characterised by the complete absence of [[magnetic permeability]] (i.e. a [[magnetic susceptibility]] <math> \chi_{v}</math> = −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#Superconductors|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. | |||
[[Image:EfektMeisnera.svg|thumb|right|Diagram of the Meissner effect. Magnetic field lines, are excluded from a superconductor when it is below its critical temperature.]] | |||
==Theory== | |||
[[Fritz London]] and [[Heinz London]] developed the theory that the exclusion of [[magnetic flux]] is brought about by [[electrical]] screening currents that flow at the surface of the superconducting material and which generate a [[magnetic field]] that exactly cancels the externally applied field inside the superconductor. These screening currents are generated whenever a superconducting material is brought inside a magnetic field. This can be understood by the fact that a superconductor has zero electrical resistance, so that "[[eddy current]]s", induced by the [[Motion (physics)|motion]] of the material inside a magnetic field, will not decay. Fritz, at the [[Royal Society]] in 1935, stated that the [[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== | |||
* [[Superfluidity]] | |||
* [[Timeline of low-temperature technology]] | |||
==References== | |||
* Shachtman, Tom, ''Absolute Zero: And the Conquest of Cold''. Houghton Mifflin Company, December 1999. ISBN 0-395-93888-0 | |||
{{magnetic states}} | |||
[[Category:Levitation]] | |||
[[Category:Magnetism]] | |||
[[Category:Superconductivity]] | |||
Revision as of 18:58, 7 October 2013
Superdiamagnetism (or perfect diamagnetism) is a phenomenon occurring in certain materials at low temperatures, characterised by the complete absence of magnetic permeability (i.e. a 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.
Theory
Fritz London and Heinz London developed the theory that the exclusion of magnetic flux is brought about by electrical screening currents that flow at the surface of the superconducting material and which generate a magnetic field that exactly cancels the externally applied field inside the superconductor. These screening currents are generated whenever a superconducting material is brought inside a magnetic field. This can be understood by the fact that a superconductor has zero electrical resistance, so that "eddy currents", induced by the motion of the material inside a magnetic field, will not decay. Fritz, at the Royal Society in 1935, stated that the 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. ISBN 0-395-93888-0