Inductance of a straight vs toroidal solenoid

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    Inductance Solenoid
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SUMMARY

The inductance of a long straight solenoid and a toroidal solenoid remains effectively the same, despite the longer magnetic path length of the straight solenoid. This conclusion arises from the long solenoid approximation, which allows the assumption that the magnetic field outside the solenoid is negligible when calculating the internal field. In contrast, a toroidal solenoid has a magnetic field that is zero outside, validating the assumption. The key factor influencing inductance is the strength of the magnetic field, not the path length.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically inductance.
  • Familiarity with Stokes' theorem and its application in electromagnetism.
  • Knowledge of Gauss' law and its implications for magnetic fields.
  • Basic concepts of solenoid design and magnetic field behavior.
NEXT STEPS
  • Explore the mathematical derivation of inductance for both straight and toroidal solenoids.
  • Study the application of Stokes' theorem in electromagnetic field calculations.
  • Investigate the implications of Gauss' law on different solenoid configurations.
  • Learn about practical applications of toroidal solenoids in electrical engineering.
USEFUL FOR

This discussion is beneficial for physics students, electrical engineers, and anyone interested in the principles of electromagnetism and solenoid design.

htg
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According to widely known formulas, the inductance of a long straight solenoid will remain practically the same if we bend it into a toroidal solenoid. It seems to be a contradiction, because the magnetic path length of a straight solenoid is more than two times greater.
 
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The path length isn't actually important. What matters is the strength of the magnetic field.

The long solenoid approximation is used because it allows a simplifying assumption that you can ignore any field outside the solenoid as trivially small when you calculate the field inside. (using Stokes theorem and curl B = mu0 J)

In the case of a toroid, the field actually IS zero outside so the assumption becomes a fact.
The difference between the two is trivial.
 
I find it strange (in the light of the Gauss' law) that the flux going through the inside of a long solenoid just comes back on the outside no matter how long the solenoid is.

In the case of a toroid, I don't think the field on the outside is zero - it is not confined to such a small volume, so its intensity is much smaller.
 

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