The magnitude of the magnetic torque on the loop

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SUMMARY

The discussion focuses on calculating the magnetic torque on a uniformly charged circular loop of radius R, rotating with angular speed omega in a uniform magnetic field B. The initial approach used the formula F=qvB, leading to Torque=T=qwR^2B, which was identified as incorrect. Participants emphasized the need to consider the varying contributions of torque from each charge element around the loop and suggested reviewing the magnetic dipole moment concept for accurate calculations.

PREREQUISITES
  • Understanding of magnetic fields and forces, specifically F=qvB
  • Knowledge of angular motion, particularly angular speed (omega)
  • Familiarity with the concept of torque and its calculation
  • Basic principles of magnetic dipole moments in current loops
NEXT STEPS
  • Review the concept of magnetic dipole moment in detail
  • Learn about integrating forces over charge distributions
  • Study the relationship between torque and angular displacement in magnetic fields
  • Explore advanced topics in electromagnetism, focusing on torque in rotating systems
USEFUL FOR

Physics students, electrical engineers, and anyone studying electromagnetism or working with rotating charged systems will benefit from this discussion.

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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