Electric Field induced by a Magnetic Field inside a Solenoid

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SUMMARY

The discussion centers on the relationship between electric fields and magnetic fields within a solenoid. It establishes that the integral around the loop does not conform to the standard differential relationship of electric fields, specifically stating that the induced electromotive force (EMF) is given by the equation \(\mathcal{E}=(E)(2 \pi r)=\pi r^2 |\frac{dB}{dt}|\). This indicates that the change in magnetic flux through the loop is the primary factor influencing the induced electric field, rather than a direct application of the fundamental relationship \(\frac{d \mathcal{E}}{ds}=E\).

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with electromagnetic induction principles
  • Knowledge of solenoid configurations and behavior
  • Basic calculus, particularly integration and differentiation
NEXT STEPS
  • Study the derivation of Faraday's Law of Induction
  • Explore the behavior of electric fields in varying magnetic fields
  • Learn about the applications of solenoids in electromagnetic devices
  • Investigate the implications of Lenz's Law in induced EMF scenarios
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism who seek to deepen their understanding of the interaction between electric and magnetic fields in solenoids.

shj
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The integral around the loop does not obey ## \frac{d \mathcal{E}}{ds}=E ##. (What you did works for ## F(x)=\int\limits_{a}^{x} f(t) \, dt ##. Then ## \frac{dF(x)}{dx}=f(x) ##. This loop integral does not have this form). Instead, the integral is evaluated as ## \mathcal{E}=(E)(2 \pi r)=\pi r^2 |\frac{dB}{dt}| ##
 
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Charles Link said:
The integral around the loop does not obey ## \frac{d \mathcal{E}}{ds}=E ##. (What you did works for ## F(x)=\int\limits_{a}^{x} f(t) \, dt ##. Then ## \frac{dF(x)}{dx}=f(x) ##. This loop integral does not have this form). Instead, the integral is evaluated as ## \mathcal{E}=(E)(2 \pi r)=\pi r^2 |\frac{dB}{dt}| ##
alright
 
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