EMF Induced by Changing Magnetic Field

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SUMMARY

The discussion centers on the electromagnetic field (EMF) induced by a changing magnetic field, specifically analyzing scenarios using Faraday's law. Two cases are presented: Case I for radii less than the magnetic field radius (##rR##). The calculations demonstrate that the electromotive force (emf) remains continuous at the boundary (##r=R##). The confusion arose from misinterpreting the diagram in Halliday's textbook, which led to a clearer understanding of the relationship between the concentric circles and Faraday loops.

PREREQUISITES
  • Understanding of Faraday's law of electromagnetic induction
  • Familiarity with the concept of electromotive force (emf)
  • Knowledge of magnetic field strength and its variations
  • Ability to interpret diagrams and mathematical expressions in physics
NEXT STEPS
  • Study the implications of Faraday's law in different geometrical configurations
  • Learn about the applications of electromotive force in electrical circuits
  • Explore the relationship between magnetic field strength and induced emf
  • Review Halliday's textbook for detailed examples of electromagnetic induction
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Physics students, educators, and professionals in electrical engineering who seek to deepen their understanding of electromagnetic induction and its practical applications.

BrandonInFlorida
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Homework Statement
This is a section of my book I don't understand, not literally homework. They (Halliday and Resnick) show a circular region containing a homogeneous magnetic field, which is increasing in strength. They then consider concentric circles within the region.

Faraday's Law states that the induced EMF around each loop is the negative of the time rate of change of the flux. They show how larger and larger circles within the circular region have larger and larger fluxes, more importantly larger and larger time rates of change of flux and, therefore, larger induced EMFs.

I'm with them so far. What I don't understand is when they say that concentric circles outside the region have zero induced EMF. It seems to me that once the circle considered becomes larger than the circular region containing the field, the flux and its time derivative remain constant for bigger and bigger circles. It doesn't fall to zero, so the induced EMF wouldn't fall to zero, according to Faraday's Law.
Relevant Equations
EMF = derivative of flux with respect to time
Can anyone show me where I'm wrong?
 
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You must be misunderstanding the premise. Are you certain H and R is not expanding the size of the circle at a constant dr/dt ?? Then their statement would be true (for constant B).
 
Let's say the circular region in which the field is non-zero has radius ##R##. Consider concentric cicles of radius ##r##. There are two cases.

Case I: ##r<R##
From Faraday's law in integral form, the result of the integration on both sides is $$E~2\pi~r=-\pi r^2\frac{dB}{dt}\implies E=-\frac{r}{2}\frac{dB}{dt}.$$Case II: ##r>R##
From Faraday's law in integral form, the result of the integration on both sides is $$E~2\pi~r=-\pi R^2\frac{dB}{dt}\implies E=-\frac{R^2}{2r}\frac{dB}{dt}.$$Clearly the emf is continuous at ##r=R.## It's hard to believe that H&R, which has been around more than 60 years, has an error like that. Can you post a legible photo of the relevant section?
 
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hutchphd said:
You must be misunderstanding the premise. Are you certain H and R is not expanding the size of the circle at a constant dr/dt ?? Then their statement would be true (for constant B).
Absolutely sure. The size of the circle is unchanging. The field strength, B, is increasing.
 
Yeah then I need to see the section in Halliday...
 
Ctrl+P or use 12th icon
 
kuruman said:
Let's say the circular region in which the field is non-zero has radius ##R##. Consider concentric cicles of radius ##r##. There are two cases.

Case I: ##r<R##
From Faraday's law in integral form, the result of the integration on both sides is $$E~2\pi~r=-\pi r^2\frac{dB}{dt}\implies E=-\frac{r}{2}\frac{dB}{dt}.$$Case II: ##r>R##
From Faraday's law in integral form, the result of the integration on both sides is $$E~2\pi~r=-\pi R^2\frac{dB}{dt}\implies E=-\frac{R^2}{2r}\frac{dB}{dt}.$$Clearly the emf is continuous at ##r=R.## It's hard to believe that H&R, which has been around more than 60 years, has an error like that. Can you post a legible photo of the relevant section?
Yes. How does one post a photo? None of these icons seems to correspond to upload photo. Maybe I can just attach it as a file.
 
hutchphd said:
Ctrl+P or use 12th icon
In going to take the photo, I found the issue. Although the book's diagram shows concentric circles both within and outside of the circular field, and although the labels #1, #2, #3, and #4 seem to correspond to those circles, they actually dont. They actually correspond to very small Farraday loops, which suddenly makes the whole thing make sense.

Thanks, guys. You never fail me.
 
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BrandonInFlorida said:
Yes. How does one post a photo? None of these icons seems to correspond to upload photo. Maybe I can just attach it as a file.
To post a photo click the link "Attach files", lower left.
 
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