Current Loop in a nonuniform magnetic field

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A current loop in a nonuniform magnetic field experiences a net force, which can be calculated using the equations F=IlxB and τ=μxB. The problem involves integrating the force on small segments of the loop, with considerations for the angle θ, which remains constant due to the loop's rotational symmetry. The confusion arises from the relationship between arc length Δs and angle Δθ, but it is clarified that the angle for the force calculation is not the same as the angle in the diagram. Ultimately, the net force can be expressed as F=2πRIBsinθ, confirming the solution's consistency. Understanding the cross-product and maintaining clarity on angles is crucial for solving the problem correctly.
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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