Current Loop in a nonuniform magnetic field

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Homework Help Overview

The problem involves a current loop in a nonuniform magnetic field, specifically examining the forces and torques acting on the loop due to the magnetic field diverging from a bar magnet. The magnetic field's angle with respect to the vertical is a key aspect of the discussion.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of force equations, considering the integration of forces on small segments of the loop. There is a focus on the implications of the magnetic field being constant and the changing angle θ for different segments of the loop.

Discussion Status

Some participants have provided guidance on using the differential form of the force equation and integrating around the loop. There is ongoing exploration of the relationship between the angle θ and the segments of the loop, with some clarification on the constancy of θ due to the loop's symmetry.

Contextual Notes

Participants note the assumption that the magnetic field is constant along the loop, despite the nonuniform nature of the field, and question the implications of this assumption on their calculations.

PEZenfuego
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Homework Statement



A nonuniform magnetic field exerts a net force on a current loop of radius R. The figure shows a magnetic field that is diverging from the end of a bar magnet. The magnetic field B at the position of the current loop makes an angle θ with respect to the vertical, as the same magnitude at each point on the current loop. (I know that I need to solve in terms of R, I, B, and θ
2013-03-15 19.24.19.jpg

Homework Equations



F=IlxB

F=IlBsinθ

τ=μxB

τ=μBsinθ

The Attempt at a Solution



I fought the urge to use the force equation after substitution 2∏r for l. Instead I examined the force on one small segment and planned to integrate. The length would be in terms of arc length Δs. The I would be a constant. It seems that the problem indicates that the magnetic field B is constant (surely that is an assumption because the distance from the magnet was not indicated, right?) I also thought that the angle should be the only thing changing (I doubt this is a double integral problem). The subscript i indicates that this is for some segment i.

So

Fi=IΔsBsinθi

The first thing that jumps out at me is that we don't have the necessary Δθ, but we do have Δs. Δs=ΔθR, but this is for a different θ, right? So, here is where I got lost and thought that something was wrong.

Next I tried relating it with torque.

τ=μBsinθ=FR
τ=IABsinθi
τ=I((2∏R^2)/(θ)/2∏B))sinθi=FR

But here again we have a different θ value, correct?

I would very much appreciate some help. Thank you!
 
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What are you supposed to solve for?
 
Net force
 
Use the differential form of your F equation above, which is
d F = I d l x B for the force on an element d l of the loop.

Then integrate around the loop - an easy integration since the force is constant everywhere around the loop.
 
I know that the answer is to be 2πRIBsinθ, but I don't see how or why.

dF=IdlxB is the same as saying dF=IΔsxB or dF=IBsinθΔs integrating yields

F=IBssinθ or F=2πRsinθ.

But doesn't the value of theta change for each segment?

Oh wait! No, it doesn't. It should remain constant as the ring has rotational symmetry. Am I correct in my reasoning here?
 
It is important to note that in the formula F = I B Δs sinθ, θ is not the same θ as given in the diagram. Remember, in the formula, sinθ is coming from a cross product of Δs and B.
 
PEZenfuego said:
I know that the answer is to be 2πRIBsinθ, but I don't see how or why.

dF=IdlxB is the same as saying dF=IΔsxB or dF=IBsinθΔs integrating yields

F=IBssinθ or F=2πRsinθ.

But doesn't the value of theta change for each segment?

Oh wait! No, it doesn't. It should remain constant as the ring has rotational symmetry. Am I correct in my reasoning here?

That is correct! And take note of what tsny says about theta. Keep track of angles when you take your cross-product!
 

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