A laboratory test for continuum theory (CT) (Q2800350)
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scientific article; zbMATH DE number 6569330
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | A laboratory test for continuum theory (CT) |
scientific article; zbMATH DE number 6569330 |
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15 April 2016
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continuum theory (CT)
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high-temperature-superconductivity
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electron pairing
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A laboratory test for continuum theory (CT) (English)
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The author suggests since the phenomenon of electrical resistivity arises because the masses of the mobile electrons interact mechanically with the lattice the resistance would fall to zero. If the aether circuiting in the electron pair is so complete that the external aether pumping and thereby the mass property of the pair vanished. Therefore, a lump of material will suddenly become lighter at the transition to superconductivity by an amount corresponding to the mass of all the electrons involved in its Cooper pairs. The fractional change of mass would be about \(1/1830\) N, where N is the mean atomic number of the material -- easily measured quantity. Another laboratory test for CT involves the deflection of a light beam passing laterally between two long plates when they are charged differentially.NEWLINENEWLINEFor the entire collection see [Zbl 1330.81018].
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0.6162093281745911
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0.5947657823562622
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0.5799097418785095
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