Time Dependent Current in a wire

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Homework Help Overview

The problem involves calculating the induced electromotive force (emf) in a conducting loop due to a time-dependent current in an infinite straight wire. The current varies over time, and the loop is positioned at a specific distance from the wire. Participants are exploring the implications of this setup on the induced emf.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the method for calculating the induced emf, with some questioning the appropriateness of using the formula ε = -dflux/dt. There is a focus on understanding the magnetic field's behavior around the wire and how it affects the flux through the loop.

Discussion Status

Some participants express confusion about the calculations and the method being used. There is a suggestion to consider the non-uniformity of the magnetic field across the loop, indicating a need for a more complex approach involving integration to accurately calculate the flux.

Contextual Notes

Participants note the lack of specific values for certain variables, such as the distance r in some calculations, which may affect the accuracy of their results. The problem's constraints and the nature of the current's variation are also under discussion.

kjlchem
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Homework Statement


An infinite straight wire carries a current I that varies with time as shown above. It increases from 0 at t = 0 to a maximum value I1 = 2.1 A at t = t1 = 14 s, remains constant at this value until t = t2 when it decreases linearly to a value I4 = -2.1 A at t = t4 = 24 s, passing through zero at t = t3 = 21.5 s. A conducting loop with sides W = 20 cm and L = 57 cm is fixed in the x-y plane at a distance d = 49 cm from the wire as shown.

What is ε1, the induced emf in the loop at time t = 7 s? Define the emf to be positive if the induced current in the loop is clockwise and negative if the current is counter-clockwise.

Homework Equations



B = μI/2∏r

Flux = B*A

-dflux/dt = ε


The Attempt at a Solution



I don't understand what I'm doing wrong with this problem.

This is what I have so far...

(dB*A)/dt= ε, A = L(W)

μ(dI)(L)W/(2∏rdt) = ε

μ=12.566*10^-7
dI = 2.1 A
L = .57 m
W = .2 m
dt=14 s.

On the left side of the box, r = .49 m and the current is negative, so the emf is positive.
On the right side of the box, r = 1.06 m and the current is positive, so the emf is negative.
Putting the 2 emf's together by subtracting the right side from the left side, I get an emf of -3.753*10^-9V.

What am I doing wrong?
 

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kjlchem said:
On the left side of the box, r = .49 m and the current is negative, so the emf is positive.
On the right side of the box, r = 1.06 m and the current is positive, so the emf is negative.
Putting the 2 emf's together by subtracting the right side from the left side, I get an emf of -3.753*10^-9V.

What am I doing wrong?
I'm not sure about the method you are using. For calculating EMF for a straight section of wire, I am only familiar with doing that for the wire moving through a magnetic field.

Since the wire loop is not moving, I think you have to use ε=-dflux/dt instead. So first I would first calculate the flux through the loop -- as a function of time, during the time interval that contains 7 s.
 
Yeah, I used ε = -dflux/dt. The flux as a function of time = μ(dI)(L)W/(2∏rdt)
 
kjlchem said:
Yeah, I used ε = -dflux/dt. The flux as a function of time = μ(dI)(L)W/(2∏rdt)
That won't work here; for one thing, there is no r given in this problem. I think I see your problem though:
kjlchem said:
Flux = B*A
That only works if B is uniform over the whole area. It isn't; B is stronger at the side of the rectangle closest to the wire, and weaker at the far side.

Instead, you'll need to do an integral to calculate the flux:
Flux = \int B \cdot dA​
 

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