Energy of a magnetic dipole in an external B field

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SUMMARY

The energy of a magnetic dipole in an external magnetic field is defined as U = m*B, contrary to the traditional U = -m*B. This distinction arises from the need to perform additional work to maintain a constant current in a current loop when moving it within the field. In statistical mechanics, using U = m*B leads to incorrect conclusions about magnetization, particularly that higher temperatures facilitate magnetization, which is inaccurate. The correct interpretation for permanent dipoles remains U = -m*B, aligning with the behavior of ferromagnetic materials driven by correlated electron spins.

PREREQUISITES
  • Understanding of magnetic dipoles and their behavior in magnetic fields
  • Familiarity with the concepts of work and energy in physics
  • Basic knowledge of statistical mechanics and magnetization
  • Awareness of the differences between current loops and permanent dipoles
NEXT STEPS
  • Study Feynman's lectures on physics, particularly volume 2, for deeper insights into magnetic dipoles
  • Explore the principles of statistical mechanics as they relate to magnetization
  • Investigate the role of correlated electron spins in ferromagnetic materials
  • Learn about the mathematical derivation of forces on magnetic dipoles, specifically F = +dU/dx
USEFUL FOR

Physicists, students of electromagnetism, and researchers in materials science focusing on magnetization and magnetic properties of materials.

kof9595995
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As in Feynman's lecture on physics vol 2, he showed that the "true energy" of a magnetic dipole(current loop) in an external B field is m*B, not -m*B. Basically the argument is if you want to pull a current loop from infinity to the final position, you must do extra work to keep the current in the loop constant. If you take this energy into account, the total energy will be m*B.
But in statistical mechanics of magnetization, if we use U=m*B instead of -m*B, we will get the opposite results,for example, we will get that the higher the temperature is, the easier to magnetize a material, which is obviously wrong.
How should I explain this?
 
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The reason is (as RF said) that twice as much energy must be provided to a current loop to keep the current constant while it is moved. Although U=+m*B for a current loop, the force on the loop is given by F=+dU/dx so the force on the loop is the same on a permanent dipole. For a permanent dipole, U=-m*B, and F=-dU/dt, giving the same formula for the force. The magnetization in ferromagnetic materials is due to correlated electron spins and not current loops, which is why U=-m*B is apprlpriate.
 
it makes sense, thanks.
 

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