Calculating Induced EMF in a Circular Region with Decreasing Magnetic Field

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Homework Help Overview

The discussion revolves around calculating the induced electromotive force (EMF) in a circular region where the magnetic field is decreasing over time. The problem involves a circular region of radius 2m and a magnetic field decreasing at a rate of 1.5T/s, with a focus on the EMF developed in a rod positioned within this region.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the use of induced electric fields and their relationship to the changing magnetic field. There are attempts to derive expressions for the electric field and EMF, with some questioning the dimensional consistency of proposed equations. Others suggest integrating the electric field along the rod and consider the geometry involved in the problem.

Discussion Status

The discussion is ongoing, with various interpretations and approaches being explored. Some participants have provided insights into the geometry of the problem and the application of Faraday's law, while others express uncertainty about certain assumptions and the clarity of the problem setup. There is no explicit consensus on the best approach yet.

Contextual Notes

Participants note potential misprints in the problem statement and discuss the implications of specific angles and geometric relationships in determining the flux through the area of interest. The discussion also highlights the complexity of integrating the electric field due to its circular nature.

Titan97
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Homework Statement


In the below figure, magnetic field is decreasing at a rate of 1.5T/s in a circular region of radius 2m. EMF developed in the rod will be?
Untitled.png


Homework Equations


$$V_{\text{induced}}=-A\frac{\mathrm{d}B}{\mathrm{d}t}$$

The Attempt at a Solution


I tried using induced electric fields. They will be concentric circles and its magnitude is given by $$E=-\frac{r^2}{R^2}\frac{\mathrm{d}B}{\mathrm{d}t}$$ (where ##r## is the radius of the circular region and ##R## is the radius of the circular electric field) I took the components of this electric field along the rod and then tried to used $$V=\int E_rdr$$ But finding ##E_r## is difficult. There will be two points on the rod which cut the circular electric field. What should be my approach?
 
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Hi Ti,

There is something wrong with ##
E=-\frac{r^2}{R^2}\frac{\mathrm{d}B}{\mathrm{d}t}\quad ## -- it doesn't fit dimensionally.
Where does it come from ?

I liked the expose here (although it ends abruptly) : it tells you magnitude and direction of the induced ##\vec E##, so all you need to do is take the component along the rod and integrate
 
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Aw snap. It's $$E=\frac{r^2}{2R}\frac{dB}{dt}$$

It comes from $$\int \vec{E}\cdot\mathrm{d}\vec{l}=-A\frac{\mathrm{d}B}{\mathrm{d}t}$$
 
And then some trigonometry and an integral and Bob's your uncle.
 
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The solution says that 1/5th of flux says through OAB. They solved the question in a single step while I am still stuck. How did they get 1/5?
 
A ?
 
The ends of rods are A and B
 
Very practical, with an A and a B for Area and magnetic field. Where is B ?
Titan97 said:
The solution says that 1/5th of flux says through OAB
Well, at least that should pin down the position of B (end of rod).
Interesting that there is a one step solution. I figured we were heading for some real work. Can you post it ? (This time I don't mind a picture...)
 
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@BvU I will post the picture soon. I don't have my Lumia with me now. My tab does not have a camera.
 
  • #11
@gracy I will post the pictures after 7:00 IST
 
  • #12
  • #13
If we can somehow prove that triangle BOX = 36 degrees.
Then yes, flux passing through AOB will be 1/5th of the total flux as 72 × 5= 360
(I am not sure though)
 
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  • #14
gracy said:
If we can somehow prove that triangle BOX = 36 degrees.
We can't prove that. It should be shown in the diagram. I guess there's a misprint?
 
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  • #15
We assume ##\angle OBA = 54^\circ## as well and proceed.

The bright idea (that I missed too o:) ) is to construct a Faraday loop BOAB where you know the induced emf and where you know the contributions from BO and AO are zero (why ? :smile: ).

It would still be interesting to carry out the integral as mentioned in post #4 -- a lot of work that should give the same result.( I use the term Faraday loop because I resent the word Faradian )

Then:
Titan97 said:
There will be two points on the rod which cut the circular electric field.
worried me. Is it clear that there is an induced E field as (for R > r) described in post #3 all over the place ?
 
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  • #16
Yes.
 
  • #17
The electric field can be determined for each r>R using Stokes law. (Draw a separate circle of radius r and let the circle and compute E which is tangent to the circle at each point.) Then you can find r as a function of ## \theta ## where each circle of radius r crosses the line. I think the trigonometric factors in computing the integral of E*ds cancel with a simple ## d\theta ## result. This longer integral approach can be shortened just by applying Stoke's law as mentioned above. It appears it doesn't even need to be a straight line path and Stokes law will give the same answer for the EMF for any path from A to B that stays outside of R.
 
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  • #18
The electric field lines cutting OA and OB will be circular in nature, hence the field direction at each point will be perpendicular to OA and OB. So, there will be no emf in OA and OB. Hence, emf is developed only in rod AB.
 
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  • #19
In post #17, I should have called the electric field E or E(r) instead of Er. (I was able to edit it.)
 

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