2 Types Of Magnetic Potential Energy

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The discussion focuses on two types of magnetic potential energy equations: U = -μ · B and U = (1/2) ∫ A · J dV. The first equation measures the mechanical work done by rotating a magnetic dipole in a uniform magnetic field, while the second is derived from the magnetic vector potential and relates to field energy. Participants seek clarification on the derivation of these equations and the meanings of the symbols involved, including U (energy), μ (magnetic moment), A (vector potential), J (current density), and V (volume). There is also a suggestion that A · J may relate to kinetic energy, whereas H · B pertains to potential energy, indicating a connection to the electromagnetic Lagrangian. Understanding these concepts requires a foundational knowledge of electromagnetism.
sawer
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There are 2 types of magnetic potential energy equations:
1. ##U = -\vec \mu \cdot \vec B##
2. ##U = \frac{1}{2} \int \mathbf{A} \cdot \mathbf{J} \, \mathrm{d}V##

- I have searched for the second equation, only can find some information in one web site. Do you know what their names are and differences?

- I see that second energy equation is derived from magnetic vector potential. But for the first equation, which potential equation is it derived from? Is it magnetic scalar potential?
 
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Please explain the symbols: U, μ, A, J, V.
 
The first equation simply measures the mechanical work done by rotating a magetic dipole μ in a uniform magnetic feld.
The second equation comes from the expression for field energy W=\int{\vec{H}\cdot\vec{B}}dV. I`m looking at the derivation from that to your equation given in Sommerfeld`s book (the only one I have handy at home) but you should find it in any upper level undergrad book.
 
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Hesch said:
Please explain the symbols: U, μ, A, J, V.
Energy, magnetic moment, vector potential, current density, volume. If you don't know what they mean, you`ll need to study a little E&M first.
 
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marcusl said:
The first equation simply measures the mechanical work done by rotating a magetic dipole μ in a uniform magnetic feld.
The second equation comes from the expression for field energy W=\int{\vec{H}\cdot\vec{B}}dV. I`m looking at the derivation from that to your equation given in Sommerfeld`s book (the only one I have handy at home) but you should find it in any upper level undergrad book.

The first part looks good, but notice that the second equation contains the current density. I think A \cdot J could be associated with the kinetic energy, and H \cdot B the potential energy. These terms appear in the electromagnetic lagrangian as the magnetic components of A^J and F^*F . I'm not sure how the various tensor elements divide into potential and kinetic energy.
 
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