A-level Physics - Faradays Law and Electromagnetic Induction

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Homework Help Overview

The discussion revolves around a problem related to Faraday's Law and electromagnetic induction, specifically focusing on the induced electromotive force (emf) as a coil enters and exits a magnetic field. Participants are examining the behavior of induced voltage over time as the coil interacts with the magnetic field.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to apply Faraday's Law to calculate the induced emf and questions the legitimacy of their method. They express uncertainty about the behavior of the induced voltage as the coil enters and exits the magnetic field, particularly regarding the graph's negative region mentioned in the mark scheme.
  • Some participants clarify that the induced voltage remains constant while the coil enters the field and discuss the implications of the coil being fully in or out of the field.
  • Others suggest considering the uniform change in flux linkage and the resulting emf as the coil moves through the field.

Discussion Status

The discussion is active, with participants providing clarifications and insights into the behavior of induced emf. While the original poster is processing the information and considering further attempts at the problem, there is no explicit consensus on all aspects of the question, particularly regarding the graph's shape and the negative region.

Contextual Notes

The original poster references specific parts of a problem set and a mark scheme, indicating that they are working within the constraints of a homework assignment. There is mention of uncertainty regarding the interpretation of the induced voltage behavior, particularly in relation to timing and the graph's characteristics.

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Homework Statement


The problem can be found http://www.drewett-gray.co.uk/alevel/ff&e/papers/ffe_04_Jun.pdf" (page 10 and 11) Question 4 part B i and ii
Mark Scheme if needed http://www.drewett-gray.co.uk/alevel/ff&e/papers/FFE_04_Jun_MS.pdf"

Homework Equations


Faradays law: The induced emf is directly proportional to the rate of change of flux linkage.
Induced EMF = flux change/time
Induced EMF = Blx/t = Blv


The Attempt at a Solution


Question 4 Part B)i
I have attempted this by following the method of a similar problem in my revision guide.
So after 0.2 seconds the coil enters the field...
Information I have:

N=1250
B=0.032 T
V=0.10 ms^-1

Induced EMF = Blv*N = 0.032*0.02*0.1*1250
=0.08 = 80mV as required
I've used this because (l*v = l * x/t which is the area cut per unit time). I know it got the right answer but I'm not sure if my method is legitimate or not.

Part B ii)
This part has been giving me real trouble.
The way I understand it there will be no reading on the voltmeter until 0.2 seconds because the coil has not entered the field.
I'm not sure what happens when it enters the field, but I think the voltage will increase as the coil enters the field, because more and more coil is cutting the field per unit time. Then once all the coil is in the field it will be constant for a while, and then will decrease as the coil leaves the field.
However the markscheme talks about having some graph in the negative region, and I'm not sure why this should be the case.
Another thing I was thinking was trying to work out the voltage at certain times to get a rough idea of the shape of the graph.


Thanks

I Like Number
 
Last edited by a moderator:
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While the coil is entering the field, the induced voltage will remain constant at that value you calculated, 80mV.
This is because the flux linking the coil is increasing uniformly as it enters the field. More and more flux links as it moves. As Faraday's Law says the emf depends on the rate of change of flux, then so long as the rate change is uniform, and it is, the emf will be constant.
When fully in the field, there is no further change in the flux linking the coil so the induced emf will be zero.
When leaving the field, the rate of change is the same as when it entered, except the flux linkage is decreasing now, not increasing. So the emf induced will again be 80mV but in the opposite direction. (ie negative)
When fully out of the field, the emf will be zero again.
 
Thank you! That made a lot of sense and I understood it :D
I'm going to mull over it, have another shot at the question a little later and let you know how I get on/ if there is anything I don't fully grasp.

Thanks once again.
 
I like number said:
Thank you! That made a lot of sense and I understood it :D
I'm going to mull over it, have another shot at the question a little later and let you know how I get on/ if there is anything I don't fully grasp.

Thanks once again.

You're welcome.
 

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