EMF Induced by Changing Magnetic Field

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Homework Help Overview

The discussion revolves around the concept of electromotive force (emf) induced by a changing magnetic field, specifically in the context of Faraday's law of electromagnetic induction. Participants are examining the implications of a circular region with a non-zero magnetic field and the behavior of emf in relation to the radius of concentric circles.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the application of Faraday's law in two cases based on the radius relative to the magnetic field region. Questions arise regarding the assumptions about the size of the circular region and the nature of the magnetic field's change.

Discussion Status

The discussion is active, with participants questioning the assumptions made in the original problem setup. Some have provided mathematical expressions derived from Faraday's law, while others seek clarification on the interpretation of diagrams in the reference material. There is a recognition of a potential misunderstanding that has been addressed, leading to a clearer understanding of the problem.

Contextual Notes

Participants note the importance of accurately interpreting the diagrams in the reference material, as discrepancies in labeling have led to confusion regarding the application of Faraday's law. The discussion also highlights the need for clarity on whether the radius of the circular region is changing or constant.

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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