Transformer with wire running through as secondary

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SUMMARY

This discussion confirms that a wire passing through a transformer can indeed induce an electric field, despite not forming a closed loop. The principles of Faraday's law apply, as the wire acts as part of a closed loop, allowing for voltage induction across its ends. The conversation references the betatron, a particle accelerator that utilizes a sinusoidal magnetic field to induce an azimuthal electric field within a vacuum chamber, demonstrating the practical application of these electromagnetic principles.

PREREQUISITES
  • Understanding of Faraday's law of electromagnetic induction
  • Familiarity with the concept of magnetic flux
  • Knowledge of particle accelerators, specifically betatrons
  • Basic principles of the Lorentz Force
NEXT STEPS
  • Research the principles of Faraday's law in greater depth
  • Explore the design and function of betatrons in particle physics
  • Study the relationship between magnetic fields and electric fields in electromagnetic systems
  • Investigate the applications of the Lorentz Force in various technologies
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism and particle acceleration will benefit from this discussion.

stephen163
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I want to confirm that I'm thinking about this in the right way...


Imagine a transformer. The primary has an integer number of turns. Now imagine the secondary has less than 1 turn, i.e., just a piece of wire passing through, forming essentially half a turn.

I know voltage is induced in this piece of wire. It doesn't form a closed loop, but faraday's law relates the induced electric field around a CLOSED loop to the time varying magnetic flux passing through the loop.

Can I assume that the wire itself forms PART of a closed loop and hence an electric field is indiced across the two ends?
 
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Yes, you are correct. Review the physics of a particle (electron) accelerator called a betatron. A sinusoidal magnetic field BA(t) is applied to the area (A = pi R2) inside a toroidal vacuum chamber of major radius R, inducing an azimuthal electric field E(t) inside the vacuum chamber of minor radius r << R, per Faraday's law. If the Bv(t) field on the vacuum chamber itself is half the average field BA(t) in the area A, the particle will be simultaneously smoothly accelerated by Faraday's law and deflected by the Lorentz Force F(t) = q[v(t) x Bv(t)] , and wlll remain inside the vacuum chamber as it is accelerated. This demonstrates that the accelerating electric field is everywhere inside the vacuum chamber.
 

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