EMF produced across one side of a coil

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Homework Help Overview

The discussion revolves around the calculation of the electromotive force (emf) produced across one side of a coil in the context of electromagnetic induction. Participants are examining the factors that influence the emf generated as the coil rotates in a magnetic field.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of maximum emf and question the relationship between the emf produced by different sides of the coil. There is exploration of the direction of induced current and its relation to the emf, as well as the reasoning behind why certain sides of the coil do not produce emf.

Discussion Status

The conversation is active with participants providing insights and questioning assumptions. Some guidance has been offered regarding the contributions of different sides of the coil to the total emf, and there is recognition of the need to clarify the conditions under which emf is induced.

Contextual Notes

Participants are navigating the complexities of Faraday's Law and the conditions required for emf induction, including the orientation of the coil relative to the magnetic field. There are references to specific parts of the original question that may influence understanding.

songoku
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Homework Statement
Please see below
Relevant Equations
ε = - N . ΔΦ / Δt
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I want to ask about part c (iii). This is what I did:

max e.m.f produced = NBAω = 32 x 0.074 x 4.8 x 10-2 x 2.4 x 10-2 x 2π x 9 = 0.15 V

But the answer is 0.077 V so my answer is off by factor of two.

Is my mistake related to "emf produced across the side of AC of the coil"?

Thanks
 
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songoku said:
max e.m.f produced = NBAω = 32 x 0.074 x 4.8 x 10-2 x 2.4 x 10-2 x 2π x 9 = 0.15 V
You might like to consider the emf (including the emf's 'direction') produced by each side of the complete coil as it rotates.
 
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Steve4Physics said:
You might like to consider the emf (including the emf's 'direction') produced by each side of the complete coil as it rotates.
By direction of emf, do you mean the direction of induced current?

If yes, then the direction of induced current is anticlockwise (viewed from above) so the current on side AC is from C to A and current on side BD is from B to D
 
songoku said:
By direction of emf, do you mean the direction of induced current?
Yes. I meant the direction from positive to negative. 'Polarity' would be a better word. And this gives the current direction.

songoku said:
If yes, then the direction of induced current is anticlockwise (viewed from above) so the current on side AC is from C to A and current on side BD is from B to D
Agreed. Note that sides AC and BD are each producing their own emf (a bit like in part C(II) of the original question). These emf sources are in series, so the total emf is their sum.

Sides AB and CD produce no emf - do you know why?

You calculated the emf produced by the whole coil - but you are only asked for the emf produced by side AC. Can you see why you got an answer double the correct answer?
 
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Steve4Physics said:
Sides AB and CD produce no emf - do you know why?
Because point A and B are at same potential and also point C and D are at same potential?

Steve4Physics said:
You calculated the emf produced by the whole coil - but you are only asked for the emf produced by side AC. Can you see why you got an answer double the correct answer?
Yes, I should divide my answer by 2
 
songoku said:
Because point A and B are at same potential and also point C and D are at same potential?
These potentials are equal as you say - but that's because AB and CDproduce no emf. It is not the reason that AB and CD produce no emf.

The potentials at, say, A and C are different because an emf is induced in AC.
The potentials at, say, A and B are the same because no emf is induced in AB.

But why should emf be induced in AC but not in AB?

songoku said:
Yes, I should divide my answer by 2
Yes. Note that it's because AC and BD produce equal emfs and AB and CD produce no emfs.
 
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Steve4Physics said:
These potentials are equal as you say - but that's because AB and CDproduce no emf. It is not the reason that AB and CD produce no emf.

The potentials at, say, A and C are different because an emf is induced in AC.
The potentials at, say, A and B are the same because no emf is induced in AB.

But why should emf be induced in AC but not in AB?
I think because AB and CD are parallel to the magnetic field so when they rotate they don't cut the magnetic field?
 
songoku said:
By direction of emf, do you mean the direction of induced current?
An unnecessary sidenote, but I find that a strange question.
They are indeed the same here, but I always think that the emf is induced and the current IF ANY is caused by that emf. Were the coil to be incomplete - with a break in AB or CD, say - then the induced emf would be the same, but there would be no current.
When calculating the current in a motor, the current will normally be in the opposite direction to the induced emf, because that current is driven by an external emf greater than the induced back-emf.
 
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songoku said:
I think because AB and CD are parallel to the magnetic field so when they rotate they don't cut the magnetic field?
AB and CD are not always parallel to the magnetic field. But, as they rotate, they do not cut through the magnetic field in the direction required to produce an emf.
 
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  • #10
There's a contractio on adjecto already in the title of this thead. An EMF is defined as an integral along a closed loop,
$$\mathcal{E}=\int_{\partial A} \mathrm{d} \vec{r} \cdot (\vec{E}+\vec{v} \times \vec{B})=-\dot{\Phi}_{\vec{B}},$$
where ##A## is a surface enclosed by its boundary ##\partial A##, with the velocity field ##\vec{v}## along this boundary, and
$$\Phi_{\vec{B}}=\int_A \mathrm{d}^2 \vec{f} \cdot \vec{B}$$
is the magnetic flux through this area.
 
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  • #11
songoku said:
I think because AB and CD are parallel to the magnetic field so when they rotate they don't cut the magnetic field?
Steve4Physics said:
AB and CD are not always parallel to the magnetic field. But, as they rotate, they do not cut through the magnetic field in the direction required to produce an emf.
Another way of looking at it is this. AB and CD rotate in planes in which the magnetic field lies entirely. One might consider a motional emf across the diameter of the rod, but that would not generate a current around the closed loop.
 
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  • #12
vanhees71 said:
There's a contractio on adjecto already in the title of this thead.
Should that be 'contradictio in adjecto'?

vanhees71 said:
An EMF is defined as an integral along a closed loop,
At an introductory level it’s common to think about emfs induced in moving straight conductors. E.g. see part C-II of the original question in Post #1.

The coil’s total emf is then the sum of the emfs from the sides. So (in the context of the question) the title doesn't seem too bad.
 
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  • #13
Thank you very much for the help and explanation Steve4Physics, Merlin3189, vanhees71, kuruman
 
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  • #14
Steve4Physics said:
Should that be 'contradictio in adjecto'?
yes, of course.
Steve4Physics said:
At an introductory level it’s common to think about emfs induced in moving straight conductors. E.g. see part C-II of the original question in Post #1.
That explains the confusion of students at the introductory level about Faraday's Law of induction.
Steve4Physics said:
The coil’s total emf is then the sum of the emfs from the sides. So (in the context of the question) the title doesn't seem too bad.
You have to take a line integral along a closed path in Faraday's Law. Anything else doesn't make mathematical sense!
 

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