How Does Mass Affect EMF in a Rotating Loop with Constant Angular Velocity?

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Homework Help Overview

The discussion revolves around a physics problem involving a rotating square loop in a magnetic field, specifically focusing on the relationship between mass, angular velocity, and electromotive force (EMF) induced in the loop. The original poster seeks to understand the relevance of the loop's mass in the context of the problem.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the expression for magnetic flux and its implications, questioning the necessity of the loop's mass in the problem. They explore the relationship between the loop's motion and the induced EMF, referencing Faraday's Law of Induction.

Discussion Status

The discussion is active, with participants providing insights into the mathematical formulation of the problem and questioning assumptions about the loop's mass. Some guidance has been offered regarding the calculation of energy dissipated in the loop, contingent on finding the EMF as a function of time.

Contextual Notes

Participants note that the loop has a resistance, which is relevant for calculating energy dissipation. There is mention of a second part to the question that may further clarify the role of mass.

eoghan
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Homework Statement


Hi! I have a problem with this exercise:
A squared loop of length L and mass M can rotate around one of its vertices and it's on a vertical plane. In the region below the suspension point there is a uniform magnetic field B perpendicular to the plane of the loop.
If the loop rotates at a constant angular velocity w, find the electromagnetically induced EMF.

Here's a picture:
http://www.allfreeportal.com/imghost/thumbs/756421Untitled1.png

The Attempt at a Solution


\phi(B)=\frac{L^2B}{2}tan(\omega t)
EMF=-\dot{\phi}(B)

Now the question: why does the text tell me the mass of the loop?:confused:
Has it something to do with the fact that the angular velocity is constant?
 
Last edited by a moderator:
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I don't think M is necessary. If there is a second part to the question, it may be relevant there.

However, you should take a second look at your expression for φ.

Based on the units you are using, φ is the magnetic flux.
\phi = \int B dA
For a uniform field and an area A inside that field,
\phi = B \int dA = B A_{inside\hspace B}

According to your φ, it goes to infinity every half period, which would imply that either L or B goes to infinity, which is not the case.

To find φ properly, it is necessary to express the area of the loop that is in the magnetic field as a function of angle, and hence a function of time. As the loop is a square, the expression may be a little complicated.

Next, Farady's Law of Induction tells us:
EMF = -\frac{d \phi}{d t} \neq -\phi

Note that when the entire loop is completely above or below the suspension point (a whole π radians of its motion per cycle), φ is constant, and hence EMF = 0.
 
Last edited:
Hao said:
I don't think M is necessary. If there is a second part to the question, it may be relevant there.

Yes, there is a second part: calculate the energy dissipated in one oscillation by the induced current.
 
I can only imagine energy being dissipated if the loop has a finite resistance.

I hope the question gives more information on what the loop is made of.
 
Last edited:
oh sorry.. the loop has a resistance R.
 
Once you have found the EMF as a function of time, you will be able to find power, and hence, by integration over one cycle, the energy dissipated.
 
Thank you!
 

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