Self inductance of a superconductor

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SUMMARY

The discussion centers on the self-inductance of superconductors, particularly how they interact with magnetic fields and Lenz's law. Superconductors exhibit unique properties, allowing them to hover above magnets due to eddy currents that oppose external forces without resistance. The concept of infinite self-inductance is addressed, clarifying that while internal currents may cancel each other, external currents remain unaffected. The coupling of current filaments on the surface of a superconductor plays a crucial role in determining self-inductance, independent of resistance.

PREREQUISITES
  • Understanding of Lenz's law
  • Knowledge of superconductivity principles
  • Familiarity with magnetic coupling in conductors
  • Basic concepts of eddy currents
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  • Research the principles of superconductivity and its applications
  • Explore the mathematical formulation of self-inductance in superconductors
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Physicists, electrical engineers, and students studying superconductivity and electromagnetism will benefit from this discussion.

greypilgrim
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Hi.

Superconductors can be made hover above or even below magnets. As far as I know, this can be interpreted as an extreme form of Lenz's law: Eddy currents on the surface of the superconductor create an opposing force that is able to cancel gravity since the currents aren't affected by resistance.

By that logic, shouldn't a superconducting coil have infinite self inductance and thereby be not conducting at all? Shouldn't turning on a current create a current of the same magnitude but opposite direction in neighboring loops so they exactly cancel?
 
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It is the internal currents that cancel. The external currents do not.
There is no problem inducing a current to flow on the surface of a superconductor. The filaments of current that flow along the surface of a superconductor are coupled to each other. Likewise other parts of the same conductor that are further away couple less. Self-inductance is a function of the magnetic coupling of the conductor to all other parts of itself, quite independent of the resistance of the conductor.
 

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