Does Faraday's Law Account for Varying Induced Flux in a Loop?

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Discussion Overview

The discussion revolves around the application of Faraday's law of electromagnetic induction, particularly in scenarios where the induced flux in a loop may vary due to the influence of both external magnetic fields and the loop's own induced currents. Participants explore the implications of self-inductance and the complexities that arise when calculating induced electromotive force (emf) in such contexts.

Discussion Character

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

Main Points Raised

  • One participant questions whether varying induced flux needs to be considered when applying Faraday's law if the induced emf itself is changing over time.
  • Another participant asserts that internal flux must be considered unless it is significantly smaller than the external flux, referencing Lenz's law to explain the directionality of the internal flux.
  • A participant introduces the concept of self-inductance as relevant to the discussion of induced emf in loops of wire.
  • There is a hypothetical scenario presented involving a complex time-dependent magnetic field, raising the difficulty of finding an expression for emf due to the contributions of both external and self-induced flux.
  • One participant expresses uncertainty about the treatment of self-induced flux and its relation to Lenz's law, questioning the sign in the total flux calculation.
  • A later reply provides a mathematical expression for emf and current in a loop, indicating conditions under which self-inductance can be neglected.
  • Another participant clarifies the distinction between internal flux due to the loop's own current and external flux.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of considering self-induced flux in calculations involving Faraday's law. There is no consensus on whether it can be ignored under certain conditions, and the discussion remains unresolved regarding the implications of varying induced flux.

Contextual Notes

Some limitations include the complexity of the mathematical expressions involved and the assumptions made about the relative magnitudes of external and internal fluxes. The discussion also highlights the dependence on specific conditions such as resistance and inductance in the loop.

kobulingam
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Faraday's law says

induced emf = - d(flux)/dt


If this is applied to a loop where induced emf causes currents, and thus flux itself, do we have to consider that flux (of course we don't if it's constant)?

If the external flux has a nonzero second derivative, then the induced emf is changing with time, thus the induced flux has a nonzero first derivative. Will this varying induced flux need to be considered when applying Faraday's law?
 
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Yes. The internal flux must be considered except where it is much smaller than the external flux. Lenz' law describes the internal flux as opposite in direction to the external. Hence the net flux decreases. Faraday's law relates the *net* flux to the emf. Thus the emf is determined by the external flux plus the geometry and resistance of the loop itself.

Claude
 
This leads to the concept of "self inductance" of a coil or loop of wire.
 
Say we have a circular loop of wire with some area and a uniform magnetic field pointing directly into it (no angle).

What if the magnitude of B is something like

B(t) = 100T^5 + 100t^4 + 100T^3 + 100T^2 + 100T + 100


Then finding an expression for emf in loop of wire will be very hard, correct?

Because the actual flux through the loop at time t is not just Area*B'(t) , but rather (Area*B'(t) + self_flux'(t) )

Where self_flux(t) is the flux created by the loop itself.

Correct?
 
I worked this problem out last month, but it's at home and I'm at work right now. I'll scan it and post it later tonight.

Claude
 
cabraham said:
I worked this problem out last month, but it's at home and I'm at work right now. I'll scan it and post it later tonight.

Claude

I just made that question up to explain the issue I'm having in understanding Faraday's law. It's not a problem from anywhere.

If you mean that you also "considered" this issue a month ago and worked out some proof where we can ignore the self_flux, then that would be great if you can scan that work.
 
kobulingam said:
Because the actual flux through the loop at time t is not just Area*B'(t) , but rather (Area*B'(t) + self_flux'(t) ) Where self_flux(t) is the flux created by the loop itself.

Correct?
Isn't there a minus sign in the total flux because of Lenz' Law?
 
Here it is. I reuploaded it in a jpg format. I forgot about the psd format being unreadable for most. The emf, or voltage if you prefer, and current, is given by:

V = -j*omega*phi_e*R / (R + j*omega*L);

I = j*omega*phi_e / (R + j*omega*L).

Plugging in all boundary conditions makes perfect sense. If R is quite large, >> omega*L, then V reduces to:

-j*omega*phi_e, which is Faraday's law w/o considering self inductance.

Note - R = resistance of loop; L = inductance of loop; phi_e = external flux normal to loop; omega = radian frequency of time changing flux.

Comments are welcome.

Claude
 

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Last edited:
Also, phi_i = internal fluz due to loop's own current.

Claude
 

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