Calculating Induced Current in an Expanding Loop

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Homework Help Overview

The problem involves a pliable round metal loop expanding in a constant magnetic field, with the aim of finding the induced current as a function of time. The loop's radius and resistance per unit length change over time, and participants are tasked with deriving the induced current based on these variables.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the calculation of induced EMF and its relationship to the changing area of the loop. There are attempts to differentiate the area with respect to time and questions about the correct application of resistance per unit length in the context of the loop's circumference.

Discussion Status

Some participants are exploring the correct expressions for induced EMF and current, with guidance provided on the differentiation process and the need to consider resistance in terms of circumference. There is acknowledgment of mistakes in earlier attempts, and clarification on terminology and mathematical expressions is ongoing.

Contextual Notes

Participants are navigating the complexities of changing geometry and resistance in the context of electromagnetic induction, with some confusion about the proper application of derivatives and terminology related to flux and area.

Andy13
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Homework Statement



Imagine a pliable round metal loop that can expand or contract. In a region with a constant magnetic field B0 that is oriented perpendicular to the plane of the loop, suppose that the loop expands, with its radius growing with time as r = r0(1+at2). As the loop expands and grows thinner, its resistance per unit length changes according to R = R0(1+bt2). Find an expression for the current induced in the loop as a function of time. To check your answer, suppose that B0 = 3.30 mT, r0 = 16.5 cm, R0 = 7.55Ohm/m, a = 0.245 x 10-4 s2, and b = 0.590 x 10-2 s2. What is the value of the induced current at t = 27.5 s? (Note: Give the direction of the current where when viewed from above a positive current will move counterclockwise.)

Homework Equations



V = IR
EMF = d(flux)/dt
flux = Sb*dA (integral of dot product of B and dA, or |B||dA|cos(90) in this case --> BdA)

The Attempt at a Solution



First, find EMF induced and then use V = IR to solve for I. This is the equation I came up with:

I(t) = B∏(ro(1+at^2))^2/(Ro(1+bt^2) = 7E-6 A

This answer wasn't correct in my online homework program. The negative value was also incorrect. Then, I reread the question and saw the part about the equation for resistance being per unit length, so I got this equation (multiply above by circumference):

I(t) = 2B∏^2(ro(1+at^2))^3/(Ro(1+bt^2) = 7E-6 A

It didn't change my answer. Which equation is right (if either)?
 
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Neither one is correct. What is the induced EMF in the loop?
 
phyzguy said:
Neither one is correct. What is the induced EMF in the loop?

Should be -d(flux)/dt = integral (B*dA)
the derivative of an integral of an equation with respect to t is just B*dA

So my mistake was to forget to differentiate at all. Whoops.

A = ∏r^2 but r= ro(1+at^2)
so dA = derivative of ∏(ro(1+at^2)^2 = 4∏*a*t*ro(1+at^2)

EMF = B*4∏*a*t*ro(1+at^2)

Does my derivative look ok? And, was I right in thinking that in order to get the resistance in the equation V = IR you have to multiply by the circumference because the equation gives resistance/unit length?
 
OK, you're on the right track now. Your derivative looks OK, except it should be r0^2. And yes, you are right that since the resistance is pre unit length, you need to multiply by the circumference.
 
phyzguy said:
OK, you're on the right track now. Your derivative looks OK, except it should be r0^2. And yes, you are right that since the resistance is pre unit length, you need to multiply by the circumference.

Thanks, got it!
 
Andy13 said:
Should be -d(flux)/dt = integral (B*dA)
the derivative of an integral of an equation with respect to t is just B*dA

The right side of this equation is the flux:

\Phi = \int \vec{B} \cdot d\vec{A}

So, after evaluating \Phi(t), you would then take its time derivative to get the emf. But to get this flux, you only need to multiply the magnetic field by the area, since

\Phi = \int \vec{B} \cdot d\vec{A} = BA

if the magnetic field is perpendicular to the area and is uniform throughout the area. Then you do

\text{emf} = -\frac{d\Phi}{dt}.

In particular, none of this needs to involve taking the derivative of the area.
 
Steely Dan said:
\Phi = \int \vec{B} \cdot d\vec{A} = BA

if the magnetic field is perpendicular to the area and is uniform throughout the area. Then you do

\text{emf} = -\frac{d\Phi}{dt}.

In particular, none of this needs to involve taking the derivative of the area.

Um...what? If B is constant, and phi = BA, then isn't d(phi)/dt = B * dA/dt? Isn't this taking the derivative of the area? What are you trying to say?
 
phyzguy said:
Um...what? If B is constant, and phi = BA, then isn't d(phi)/dt = B * dA/dt? Isn't this taking the derivative of the area? What are you trying to say?

I'm correcting the OP's terminology. It looks like he has the correct expression for the magnitude of the emf but seems confused on the proper derivative and naming conventions.
 

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