What EMF is induced in the loop at t=0?

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Homework Help Overview

The discussion revolves around the induced electromotive force (EMF) in a wire loop when a current in a long cable is switched off at time t=0. The problem involves concepts from electromagnetism, particularly the behavior of magnetic fields and inductance in relation to changing currents.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the calculation of magnetic flux and induced EMF, questioning the assumptions about the current's behavior at t=0. Some suggest using Ampere's Law for a more accurate approach, while others discuss the effects of the cable's configuration on the magnetic field.

Discussion Status

There is an ongoing examination of the information provided in the problem, with participants expressing uncertainty about the adequacy of the details given, particularly regarding the physical dimensions and characteristics of the wire loop. Some guidance has been offered regarding the nature of the magnetic field and its collapse when the current is turned off.

Contextual Notes

Participants note the potential need for additional information, such as the inductance and parasitic capacitance of the wire loop, to fully address the problem. There is also mention of the load that the device might still draw after the circuit is de-energized, which could affect the induced current.

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Homework Statement


A current of 10A is switched off at time t = 0 in a long cable (picture in attachments). It powers a device, with the current return wire having 5 mm separation. A wire loop of dimension 5 by 5 cm is located at a distance 3 cm from the cable.

1) What Emf is induced in the loop at t = 0 if it is in the same plane as the wires in the cable?

2) What direction would the induced current flow in the loop?

3) What Emf would be induced if the cable were rotated 90 degrees but otherwise not moved?

Homework Equations


emf = - N ΔΦB/Δt
B = μ0 I / 2πd
ΦB = B*Area

The Attempt at a Solution



B[/B] = (4*π*10-7)*(10A) / (2*π*(0.03))
B = 6.67 * 10-5 T

ΦB = 6.67 * 10-5 * (0.052)
ΦB = 1.67 * 10-7 Wb

This is where I'm a bit confused. The question asks for the emf at t=0. I assumed that because the current is 10 A, that at t=1 second, the current will be 10A.

emf = (-1) (1.67 * 10-7) / (1)
emf = -1.67 * 10-7 V
 

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They tell you that the power is turned off at t=0, so you know that whatever flux was there, is going to start collapsing. The long conductor and its return wire will act like a 1 Turn inductor.
 
I think it might be better to use Ampere's Law: ∫B dl to solve this problem.

Won't the cable that is further away from the loop cancel out some of the magnetic field because the current is going in the opposite direction?
 
Is there enough information in the question?
 
B = μ0 I / 2πs

I've changed the d to an s from my original equation.

B ds = ∫ (μ0 I / 2πs) ds

Then I could just compute 2 integrals with different boundary conditions.
 
says said:
Won't the cable that is further away from the loop cancel out some of the magnetic field because the current is going in the opposite direction?
Yes. When computing the initial flux through the loop at time t=0-, you subtract the fields generated by the two currents.
scottdave said:
They tell you that the power is turned off at t=0, so you know that whatever flux was there, is going to start collapsing. The long conductor and its return wire will act like a 1 Turn inductor.
But the inductance and parasitic capacitance of that long wire loop will determine the amplitude and frequency of the flyback ringout waveform. They do not seem to have supplied that, unless the OP is leaving some information out of his post.
Dadface said:
Is there enough information in the question?
I don't think so either. We need the physical dimensions of the long wire loop and some way to approximate its L and parasitic capacitance in order to calculate what the loop current does after the switch is opened at t=0, IMO.
 
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I agree that we do not have enough information. For instance, we know that it powers a device, so it could still draw a load for a moment, after the circuit is deenergized.
 

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