Am I doing this torque on dipole problem right?

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    Dipole Torque
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SUMMARY

The discussion focuses on calculating the torque exerted on a square current-carrying loop by a circular loop with a steady current I. The key equations used include the torque on a dipole in a magnetic field, expressed as τ = B x m, where m is the dipole moment of the square loop. The final torque derived is N = -I²ua²b²/(4r³) in the x-hat direction, indicating that the square loop will rotate until it is antiparallel to the circular loop's magnetic moment, ultimately reaching a stable orientation with no net torque.

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Homework Statement



You've got a circular loop with a steady current I and radius 'a' a distance r from a square current carrying loop with sides of 'b' and current I, r >>> a or b(and they're arranged in such a way as you can think of the circular loop's dipole as pointing up, and the square loop point right)

What's the torque ON the square loop caused by the circular loop, and the square loop's final orientation assuming it's free to move

Homework Equations


A couple of ways to get B, I figure the curl of A, and I have A for a dipole, which will I use with the circular loop

Then the torque on a dipole in a B field is B x m, where m is the dipole, in this case the square loop's dipole

Err, I guess that was my attempt pretty much, I just need to make sure that's the right way to do it
 
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Just a thought here, buuuut isn't the B field of a circular current just a straight line going through its center(orientated with the right hand rule)? So...would there even be a torque on the square loop?

Edit: No wait that's totally wrong
 
Last edited:
Think I got it, I'll just put in my own work for shiggles

Well no, I don't know Latex worth a damn, suffice it to say I used the formula for B for a magnetic dipole sensed by another dipole, with the angle between them being pi/2, and ultimately I got

N=-I^2ua^2b^2/(4r^3) in the x-hat direction, which I believe means it'd rotate until it was antiparallel with the circular loop's moment, then theta =0, and no more torque(though I guess technically it'd swing past but blah blah ultimately they're anti-aligned?)
 
The magnetic dipole moment of each loop is just mu=IXarea/c (in gaussian units). Then, the torque is calculated just as if they were electric dipoles.
torque=muXB, where B is torque due to the other dipole.
 

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