How is the Total Energy of a Magnetic Field in Matter Calculated?

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SUMMARY

The total energy of a magnetic field in matter is calculated using the formula \(\frac{\mu H^2}{2}\). To determine the energy spent on magnetizing the material, one must subtract the magnetic field energy \(\frac{B^2}{2}\) and the dipolar interaction \(-\vec{M} \cdot \vec{B}\). The discrepancy arises because the energy density of the magnetic field is expressed as \(\frac{H^2}{2}\) rather than \(\frac{B^2}{2}\), which is a distinct approach compared to electric fields, where the energy density is \(\frac{E^2}{2}\). This difference is attributed to the definitions of H, B, and \(\mu\) and the unique interactions of matter with magnetic fields.

PREREQUISITES
  • Understanding of magnetic field concepts, specifically \(\mu\), H, and B.
  • Familiarity with energy density equations in electromagnetism.
  • Knowledge of dipolar interactions in magnetic materials.
  • Basic comprehension of the differences between magnetic and electric field equations.
NEXT STEPS
  • Study the derivation of the energy density formulas for magnetic fields.
  • Explore the implications of using different systems of units, such as cgs and SI.
  • Investigate the behavior of magnetic materials under varying magnetic field strengths.
  • Learn about the relationship between magnetic susceptibility and energy calculations.
USEFUL FOR

Physicists, electrical engineers, and materials scientists interested in the calculations and principles governing magnetic fields in materials.

LayMuon
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The total energy of the magnetic field in the matter is \frac{\mu H^2}{2}, I want to calculated the energy that is being spent as a the work on magnetizing the material, so I need to subtract the energy of the magnetic field itself \frac{B^2}{2} and the dipolar interaction -\vec{M} \cdot \vec{B}, however here is the problem $$ \frac{\mu H^2}{2} - \frac{B^2}{2} = \frac{\mu H^2}{2} - \frac{(\mu H)^2}{2} < 0 $$ for \mu &gt; &gt; 1.

Why the energy of magnetic field itself is given by \frac{ H^2}{2} and not by \frac{ B^2}{2}?
 
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That equation is for the energy density of the field, not the total energy.
And it doesn't matter if you write \frac{\mu H^2}{2} or \frac{B^2}{2\mu} because B = \mu H
 
That all was implied.

The question is why should we take the self energy density of the magnetic field as H^2/2 and not B^2/2, unlike the electric field where it is E^2/2 and not D^2/2.
 
Why do you keep writing \frac{H^2}{2} instead of \frac{\mu H^2}{2}?
Anyway, That's due to the way H, B and \mu are defined. And because matter often interacts with magnetic fields in a way that's opposite to how it interacts with electric fields.
If you use different definitions, the equations look different.
e.g. in the cgs system the equations are \frac{B^2}{8\pi} and \frac{E^2}{8\pi}
 

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