Definition of magnetic moments and torques

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SUMMARY

The discussion centers on the definition of magnetic moments and torques in the context of current loops. The torque on a rectangular current loop is expressed as \(\vec m \times \vec B\), where \(\vec m\) is the magnetic moment. The user seeks to generalize this to arbitrary current loops and questions the factor of one-half in the magnetic moment definition found on Wikipedia. The resolution involves recognizing that the factor of one-half is necessary for accurate area calculations, which ultimately affects torque calculations.

PREREQUISITES
  • Understanding of magnetic moments and torques
  • Familiarity with vector calculus and cross products
  • Knowledge of current loops and their properties
  • Basic principles of electromagnetism
NEXT STEPS
  • Study the derivation of magnetic moments for various current loop geometries
  • Explore the implications of the factor of one-half in magnetic moment calculations
  • Learn about the mathematical identities involving vector cross products
  • Investigate the relationship between torque and magnetic moment in different electromagnetic contexts
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Students and professionals in physics, electrical engineering, and applied mathematics who are interested in the principles of electromagnetism and the behavior of magnetic fields in relation to current-carrying loops.

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When one finds the torque on a rectangular current loop one finds that it's equal to

\vec m \times \vec B

where m is the magnetic moment of the loop. I want to generalize this to arbirary current loops with constant current and I found that the torque would be equal to

\left(I\oint \vec r \times \vec dl\right) \times \vec B

so I would think it would be natural to define

\vec m =I\oint \vec r \times \vec dl

for these current loops. However when it up at http://en.wikipedia.org/wiki/Magnetic_moment" I find that the magnetic moment is defined as

\vec m =\frac{1}{2} I\oint \vec r \times \vec dl.

Where does this factor of a half come into the picture? Is'nt 'moments' supposed to be that what generates torques and not just be proportional to it?
 
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Look closely at your formula, does it give the right area when you take for example a circle? (The factor 1/2 is needed to calculate the area correctly)
 
That's true. But I do not want the right area, just the right torque. I must admit I am a bit confused. I just saw a derivation of a statement that

\vec r \times (d\vec r \times \vec B) = \frac{1}{2} \left( d\left[ \vec r \times ( \vec r \times \vec B\right] - \vec B \times ( \vec r \times d \vec r ) \right)

Which would indeed solve the problem. But does this then imply that

\oint \vec r \times (d\vec r \times \vec B) = \frac{1}{2} \oint \left( d\left[ \vec r \times ( \vec r \times \vec B\right] - \vec B \times ( \vec r \times d \vec r ) \right) = \frac{1}{2} (\oint \vec r \times d \vec r) \times \vec B?

if so that would imply that

\oint \vec r \times ( d \vec r \times \vec B ) - \frac{1}2 (\vec r \times d \vec r) \times \vec B = 0

and can we not then conclude that

\vec r \times ( d \vec r \times \vec B ) = \frac{1}2 (\vec r \times d \vec r) \times \vec B?

which seems to be a contradiction when I would think that

\vec A \times ( \vec B \times \vec C) = (\vec A \times \vec B) \times \vec C.

I would really appreciate if someone could enligthen me.
 
When two integrals are the same, that does not necessarily mean the integrated functions are the same. Also, in general Ax(BxC) is not equal to (AxB)xC, always watch out with that. (these are just general remarks)

How did you arrive at your first expression for the torque? (in post #1)

edit: I was a little too fast with this reply, I should add that in this case of course you need the factor 1/2 to get to the right answer, and therefore you will need some identity ;). I suspect you (mis)used that Ax(BxC) = (AxB)xC for your first result?
 
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You're right! That exactly what I did. And that solves my problem. Thank you! :)
 

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