Induced Current Problem(Electromagnetism)

AI Thread Summary
The discussion focuses on calculating the induced current in a small circular loop placed at the center of a larger circular loop with changing current. The key equations involved include the relationship between induced electromotive force (ε), resistance (R), and magnetic flux (Φ). Participants highlight the importance of considering the area of the smaller loop when calculating the magnetic flux, as the initial calculations incorrectly applied the flux through the larger loop's area. The correct approach involves using the magnetic field at the center of the larger loop and applying it to the area of the smaller loop. Ultimately, the participant successfully resolves their misunderstanding and arrives at the correct solution.
pjwasz
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Homework Statement


A small, 1.60-mm-diameter circular loop with R = 1.40×10−2Ω is at the center of a large 120-mm-diameter circular loop. Both loops lie in the same plane. The current in the outer loop changes from 1 A to -1 A in 8.00×10−2 s.

What is the induced current in the inner loop?

Homework Equations


I = ε/R
d\Phi/dt = ε
\Phi = BAcos(0) = BA
B = (μ_0)(I)/2r

The Attempt at a Solution



First, I got (μ_0)(I)(\pi)(r)(1/2) = \Phi, using \pir^2 as A.

Then, d\Phi/dt = (μ_0)(\pi)(r)(1/2)(dI/dt)

So...I = ((μ_0)(\pi)(r)(1/2)(dI/dt))/R

Which is ((4*10^(-7))(\pi)^2(.03)(2/.08))/.014.

My answer I got was 2.11 *10^-4 A.Please help, thank you. :)
 
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It looks to me like you did not consider the smaller area of the inside loop.
 
I think you need to multiply your answer by the area of the small loop and you will get what I did.
 
pjwasz said:

Homework Statement


A small, 1.60-mm-diameter circular loop with R = 1.40×10−2Ω is at the center of a large 120-mm-diameter circular loop. Both loops lie in the same plane. The current in the outer loop changes from 1 A to -1 A in 8.00×10−2 s.

What is the induced current in the inner loop?


Homework Equations


I = ε/R
d\Phi/dt = ε
\Phi = BAcos(0) = BA
B = (μ_0)(I)/2r

The Attempt at a Solution



First, I got (μ_0)(I)(\pi)(r)(1/2) = \Phi, using \pir^2 as A.
Where did this come from?
You need to compute B in the middle of the large loop. Computing flux thruout the area of the larger loop is both nearly impossible and pointless. Your small loop sees only the B field near the center of the large loop, and fortunately this is easy to calculate using Biot-Savart law.

EDIT: as barryj pointed out, you already had the correct value for B in your equations list. So use it!
 
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I think he did compute B in the center . It seems he did not consider the smaller area of the inner loop.
 
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I think this is incorrect "First, I got (μ_0)(I)(π)(r)(1/2) = Φ, using πr^2 as A"
You have to consider the R of the big loop and the r of the small loop.

Big R = .06m and little r = .0008m

Phi = uI/2R X (pi)r^2
 
Ah, I see. So what I was doing was calculated the flux due to the magnetic field of the big loop, but through the big loop itself. Instead, I need to calculate the flux due to the magnetic field of the big loop, but through the small loop.

...Good news, that worked! Thanks guys, I get what I was doing wrong! :)
 
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