The magnitude of the magnetic torque on the loop

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Homework Help Overview

The discussion revolves around calculating the magnitude of the magnetic torque on a circular loop with a uniformly distributed positive charge, which is rotating in a uniform magnetic field. The problem involves concepts from electromagnetism, particularly relating to magnetic forces and torques on charged loops.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the relationship between force, velocity, and magnetic field, with attempts to derive torque from these quantities. There are questions about the contributions of different elements of charge to the overall torque and the need to consider varying distances from the axis of rotation.

Discussion Status

The discussion is ongoing, with participants sharing their calculations and questioning the correctness of their approaches. Some guidance has been offered regarding the magnetic dipole moment and the need for integration to account for varying distances in torque contributions.

Contextual Notes

Participants are grappling with the implications of their assumptions about charge distribution and the geometry of the loop. There is a recognition that the torque contributions may not be uniform across the loop, and some participants express uncertainty about constants in their calculations.

marpple
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A plastic circular loop of radius R and a positive charge q is distributed uniformly around the circumference of the loop. The loop is then rotated around its central axis, perpendicular to the plane of the loop, with angular speed omega.

If the loop is in a region where there is a uniform magnetic field B directed parallel to the plane of the loop, calculate the magnitude of the magnetic torque on the loop.


well, i did this
F=qvB
and know that v = w(omega).R
it gives me F=qwRB
and Torque = F. L, then i got T=qwR^2B


my answer seems not correct.., please advise.
 
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marpple said:
well, i did this
F=qvB
That's the force on a moving point charge (magnitude only) where v and B are perpendicular.
and know that v = w(omega).R
OK.
it gives me F=qwRB
Don't lump all the charge together.
and Torque = F. L, then i got T=qwR^2B
Note that the force on each element of charge on the loop will give rise to a different torque contribution, since the distance to the axis (a diameter) is different.

Hint: Review the concept of magnetic dipole moment of a current loop and the torque it experiences in a magnetic field.
 
I got close...

r varies from 0 to R
F=(q/2R*pi)Bv
v=omega*r
dtorque=(q*omega*r^2*B)/(2*pi*R)

torque= (some constant)(q*omega*B*R^2)/(3*pi)

I can't figure out the constant though. Have I only found the upper half of the loop?
 
wait no, I lost a 2. That still doesn't give me the right answer though.
 
supacalafrg said:
I got close...

r varies from 0 to R
F=(q/2R*pi)Bv
v=omega*r
dtorque=(q*omega*r^2*B)/(2*pi*R)
To solve it properly using dF = dq v X B requires taking the angle into consideration and integrating. I recommend the hint I gave in my last post.
 

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