Why is there an induced EMF in this case?

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Discussion Overview

The discussion revolves around the induction of electromotive force (EMF) in a loop moving perpendicular to a uniform magnetic field. Participants explore the conditions under which EMF is induced, the role of magnetic flux, and the implications of Faraday's Law. The conversation includes theoretical considerations, conceptual clarifications, and challenges to various viewpoints.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why an EMF is induced if the magnetic flux through the loop remains constant, suggesting that d(phi)/dt is zero.
  • Another participant asks whether the loop remains completely within the magnetic field, indicating that if it does, there should be no induced EMF.
  • A participant proposes that while there may be no net EMF in the loop, there could be equal and opposite EMFs on opposite sides of the loop due to motion.
  • Discussion arises about the induction of EMF in a straight conductor moving in a magnetic field, with some asserting it is due to the Lorentz force rather than a change in flux.
  • Contradictory views emerge regarding whether the induced EMF in a moving conductor is due to a change in flux or the movement of charges in the magnetic field.
  • Participants reference Faraday's Law and its application to closed paths, with some expressing confusion over its implications for open paths.
  • Clarifications are made regarding the nature of motional EMF and the conditions under which it arises, emphasizing the role of Lorentz forces on charges.
  • One participant reiterates that if a loop is entirely within a uniform magnetic field and moves perpendicularly, there should be no EMF due to constant flux.

Areas of Agreement / Disagreement

Participants express differing views on the conditions for EMF induction, particularly regarding the role of magnetic flux and the applicability of Faraday's Law. There is no consensus on whether the induced EMF is due to changes in flux or the motion of charges.

Contextual Notes

Limitations in understanding arise from the interpretation of Faraday's Law, particularly concerning open versus closed paths. The discussion highlights the complexity of applying theoretical principles to practical scenarios.

Salman72
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Hey people

I was wondering why is an emf induced in a loop which moves perpendicular to a uniform magnetic field. I mean, say the loop is a square of area r^2, and moves in the xy plane, where there is a uniform magnetic field B in the z direction. Why will an emf be induced? The flux remains constant right? So if d(phi)/dt is 0, why is an EMF still induced??

Thanks
 
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Does the loop remain completely inside the region where the B field exists? Or, to put it another way, does the B field always "fill" the loop? If this is true, then you are correct, there should be no induced EMF. Can you describe the example or situation that claims there is an EMF?
 
Thanks a lot!

Yes, the loop does remain completely within the field. It was just "coming" to my mind that an emf will be induced... however, I think it was because of a flawed intuition!... Anyway, will it be right to conclude that there will be no net EMF in the loop, but there will be equal and opposite EMFs (given by Blv) in the opposite sides of the loop?

And on a related note: If I move a straight piece of conductor in a uniform magnetic field, again an EMF is induced (proved using B*l*v I think). However, where is the flux change in that? I mean, there is no flux to begin with, since there is no loop- so how can we prove the EMF using Faradays Law?
 
Salman72 said:
Thanks a lot!

Yes, the loop does remain completely within the field. It was just "coming" to my mind that an emf will be induced... however, I think it was because of a flawed intuition!... Anyway, will it be right to conclude that there will be no net EMF in the loop, but there will be equal and opposite EMFs (given by Blv) in the opposite sides of the loop?

And on a related note: If I move a straight piece of conductor in a uniform magnetic field, again an EMF is induced (proved using B*l*v I think). However, where is the flux change in that? I mean, there is no flux to begin with, since there is no loop- so how can we prove the EMF using Faradays Law?
If a straight conducting rod is moving in a uniform magnetic field, in a direction perpendicular to the field, the induced emf is not due to a change in flux. It is because charges collect at the edges because of the Lorentz force. This is called motional emf.
 
Chandra Prayaga said:
If a straight conducting rod is moving in a uniform magnetic field, in a direction perpendicular to the field, the induced emf is not due to a change in flux. It is because charges collect at the edges because of the Lorentz force. This is called motional emf.

But it is due to a change in flux. The conducting rod forms only one part of the circuit that forms a complete loop.
 
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stedwards said:
But it is due to a change in flux. The conducting rod forms only one part of the circuit that forms a complete loop.

No, it is due to charges moving in a magnetic field. Change in flux is a rule of thumb. Notice that if the charges all move in one direction (i.e. down, not clockwise) then the emfs of each half of the loop will cancel. You'll just have some charges collecting at the top/bottom of the loop.
 
crador said:
No, it is due to charges moving in a magnetic field. Change in flux is a rule of thumb. Notice that if the charges all move in one direction (i.e. down, not clockwise) then the emfs of each half of the loop will cancel. You'll just have some charges collecting at the top/bottom of the loop.

I have no idea what any of this means. Apparently Faradays Law \oint E \cdot s +d\Phi_{B}/dt is a "rule of thumb".
 
Faraday's Law in integral form requires a closed path. It can't be applied to an open path.
 
jtbell said:
Faraday's Law in integral form requires a closed path. It can't be applied to an open path.

Yes, that's why I used the \oint. The open path wasn't made clear to me in the post. Thanks for clarifying.
 
  • #10
stedwards said:
I have no idea what any of this means. Apparently Faradays Law \oint E \cdot s +d\Phi_{B}/dt is a "rule of thumb".

What this means is that the physics is simply about moving charges in magnetic fields.

Yes, apparently Faraday's Law is a rule of thumb, since it only describes conveniently closed paths. Do you think the physics breaks down if I only look at each half of the path independantly?
 
  • #11
crador said:
What this means is that the physics is simply about moving charges in magnetic fields.

Yes, apparently Faraday's Law is a rule of thumb, since it only describes conveniently closed paths. Do you think the physics breaks down if I only look at each half of the path independantly?

Again, say what you mean. I'm not a mind reader. Do you have anything to add beyond what jtbell said?
 
  • #12
stedwards said:
Again, say what you mean. I'm not a mind reader. Do you have anything to add beyond what jtbell said?

I suppose I am not being eloquent enough for you. My apologies.

I am trying to make you get it, namely that Faraday's Law is a rule of thumb for predicting the net result of the Lorentz forces on the charged particles in a closed loop of conducting material. This is not much beyond what jtbell and Chandra said, but it seemed like you were still having difficulty in accepting it.

To re-illustrate the example I used: Say you have a uniform magnetic field pointing out of the page everywhere. If you drag a loop of conducting wire that is normally oriented to it towards the right, there will be a downward force on the positive charges, and an upward force on the negative ones, as per the Lorentz force law.

The charges will migrate up and down respectively, establishing an electric field that will balance the effect of the magnetic field and movement, i.e. charges will migrate until the Lorentz force F = q [ E + v x B ] is equal to zero.

So you will have a motional emf as Chandra said, a voltage difference between the top and bottom of the loop. You will not have an emf around the circuit though, since the endpoints of any closed path will have the same voltage. This is the meaning of Faraday's Law, as jtbell said: it only applies to the whole closed loop -- when flux is constant as in this case there is no net emf around the loop.

I hope that helps!
 
  • #13
stedwards said:
But it is due to a change in flux. The conducting rod forms only one part of the circuit that forms a complete loop.
If it is a complete loop, and the loop is entirely within the uniform magnetic field, moving the loop in a direction perpendicular to the magnetic field does not change the flux, and there is no EMF. EMF is there only if the flux changes, as stated in Faraday's law.
 

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