Is It Incorrect to Use ∫E . dr in a Moving Conductor?

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Discussion Overview

The discussion revolves around the application of Faraday's law of electromagnetic induction, particularly the use of the integral ∫E . dr in the context of a moving conductor within a magnetic field. Participants explore the relationship between induced electromotive force (EMF), potential difference (PD), and the path dependency of electric potential in both conservative and non-conservative fields.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the EMF induced in a closed loop is given by -d(phi)/dt, questioning the specific points between which this potential difference is measured.
  • Others illustrate the concept using analogies of batteries in a circuit to explain how potential difference can be perceived between any two points in a loop.
  • There is a discussion on whether electric potential difference is conservative, with some arguing that it is path-dependent in the context of time-varying electric fields.
  • One participant notes that the potential around a closed loop requires work to transport charge, suggesting that the potential is not simply additive in cases of varying fields.
  • Concerns are raised about the implications of measuring EMF across infinitesimally close points and how that relates to practical scenarios involving resistance and induced currents.
  • Participants question the apparent contradictions when applying these concepts to specific problems involving moving conductors and fixed loops.
  • There is a mention of Lenz's law and its effect on the induced EMF and current in circuits with varying resistance.

Areas of Agreement / Disagreement

Participants express differing views on the nature of electric potential difference, particularly regarding its conservativeness and the implications of using infinitesimal segments for calculations. The discussion remains unresolved, with multiple competing perspectives on the relationship between EMF, PD, and the path taken in a circuit.

Contextual Notes

Limitations include the dependence on specific configurations of circuits and the assumptions made about resistance and induced currents. The discussion highlights the complexity of applying theoretical principles to practical scenarios.

  • #31
There is nothing wrong per se, it's just that in a circuit problem, for example you're usually not given the electric field vector function so you can't use that.
 
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  • #32
anantchowdhary said:
And how can we apply Kirchoff's Loop Law in an LR circuit as there is a non conservative electric field induced in the solenoid?
and can anyone please confirm that is emf defined by
E . dr
starting from ANY point and ending at the same point on the loop
even in a moving conductor
Defennder said:
Kirchoff's voltage law still applies here. Although the electric field is non-conversative, the drop in potential across any circuit loop is still 0 …
anantchowdhary said:
Is there anything wrong in using
E . dr
Hi anantchowdhary! :smile:

Both versions are correct!

The induced emf, from Faraday's Law, isE . dr, and it is measured starting from ANY point and ending at the same point on the loop.

On the other hand, the drop in potential across the loop … between the same two points … is zero.

In the first case, you're only measuring the induced emf.

In the second case, you're measuring the induced emf and the voltage drops.

If the loop is just a wire, with nothing added, then the emf is ∫E . dr, starting from any point and ending at the same point.

But the wire has resistance, so there's an IR to balance it, and that IR is also spread around the whole loop.

Now insert a light bulb, or a voltmeter, anywhere the loop … suddenly 99.999% of the resistance is now in the bulb or voltmeter, so the emf is 99.999% of E . dr, from one end of the bulb to the other.
 

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