What is the Demagnetizing Field in Magnetism?

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SUMMARY

The discussion centers on the concept of the demagnetizing field (NM) in magnetism, particularly in relation to the B and H fields. The relationship is defined by the equation H = B/u - M, where the internal H field (Hi) is expressed as Hi = Ha - NM. The demagnetizing field arises from the induced magnetization (M) in ferromagnetic materials, which opposes the external H field, thereby reducing the overall magnetization. This phenomenon is illustrated using an iron cylinder subjected to an external magnetic field (H_0), where boundary conditions lead to an effective magnetic charge density that visualizes the demagnetizing effect.

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  • Understanding of magnetic fields, specifically B and H fields.
  • Familiarity with the concepts of magnetization (M) and demagnetization.
  • Knowledge of boundary conditions in electromagnetic theory.
  • Basic grasp of ferromagnetic materials and their behavior in external magnetic fields.
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  • Study the mathematical derivation of the demagnetizing field in ferromagnetic materials.
  • Explore the applications of boundary condition equations in magnetostatics.
  • Learn about the effects of demagnetization on magnetic materials in practical scenarios.
  • Investigate the role of magnetic charge density in the context of magnetism.
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Physicists, electrical engineers, and materials scientists interested in the principles of magnetism and the behavior of ferromagnetic materials under external magnetic fields.

Master J
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So I understand what the B field is in magnetism. This is the fundamental field.

We can also define a H field, H = B/u - M, to take into account that we cannot actually measure magnetization currents (cf. solenoid).

Now, if we have a B field applied to a material, call it Ba, the field inside is given by

B = u(Hi + M), where Hi is the internal H field, defined as Hi = Ha - NM. Its this last part that confuses me. What is this demagnetizing field, NM?
 
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Most writers state that the magnetism in a ferromagnetic object is induced by an external H (not B) field. To visualize the demagnetizing field, imagine an iron cylinder with its axis parallel to a field H_0. Boundary condition equations allow one to replace the induced M by an effective (and fictitious) magnetic charge density on the face of each end. The field outside the rod is that from the two charged surfaces (this field appears dipolar at sufficient distances) added to H_0. Note that inside the rod the charges produce a field that opposes the external field, tending to reduce M. This is the demagnetizing field.
 

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