Magnetic Moment Definition Verification/ Proof

AI Thread Summary
The equation for the magnetic moment of a non-planar loop, m = (I/2) ∫ r × dr, is a convenient definition used to approximate the magnetic field generated by currents at large distances. This definition helps assign a magnetic moment to a region of space where currents flow. For derivations and proofs, refer to D.J. Griffiths' "Introduction to Electrodynamics" and J.D. Jackson's "Classical Electrodynamics," which provide detailed explanations. The derivation of the magnetic moment equation is typically covered in one page of standard electromagnetism textbooks. Understanding this equation is essential for grasping the behavior of magnetic fields produced by current loops.
cubejunkies
Messages
33
Reaction score
0
I saw the equation here http://en.wikipedia.org/wiki/Magnetic_moment#Current_loop_definition for the definition of the magnetic moment for a non-planar loop. Can someone tell me if there's a name for this equation m= \frac { I }{ 2 } \int { \overrightarrow { r } } \times d\overrightarrow { r }, if it's even right, and where I could find a derivation and/or proof of the equation? I've been fumbling over this for several hours now and I've gotten absolutely nowhere. I don't have any access to any texts on the matter, all I have is google and wikipedia at the moment.

Thanks

Anthony
 
Physics news on Phys.org
It is really just a convenient definition. It assigns to some portion space (where the currents are) a quantity called magnetic moment. The motivation is, we want to find some approximate expression for the magnetic field due to these currents, and it turns out that in large distances, the magnetic moment is sufficient to find it. Try to get and look into D.J. Griffiths, Introduction to electrodynamics, sec. 5.4.3 or J.D. Jackson: Classical Electrodynamics, you should find the details there.
 
It follows from
{\bf m}=\frac{1}{2}\int{\bf r\times j}d^3r
with the substitution {\bf j}d^3r\rightarrow I{\bf dr}.
The derivation of the j equation takes about one page in an EM textbook.
It is on J. Franklin, "Classical Electromagnetism" on page 212.
Your equation is derived directly on page 210.
You should also know that \frac{1}{2}\int{\bf r\times dr}=
the area of the loop.
 
Last edited:
Thread 'Motional EMF in Faraday disc, co-rotating magnet axial mean flux'
So here is the motional EMF formula. Now I understand the standard Faraday paradox that an axis symmetric field source (like a speaker motor ring magnet) has a magnetic field that is frame invariant under rotation around axis of symmetry. The field is static whether you rotate the magnet or not. So far so good. What puzzles me is this , there is a term average magnetic flux or "azimuthal mean" , this term describes the average magnetic field through the area swept by the rotating Faraday...
Back
Top