5) Zeeman energy

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Last updated 10:34 AM on 6/10/26
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12 Terms

1
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What is the Zeeman energy

energy associated with aligning the magnetic moment with the field

2
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Zeeman energy equation

E_z = -μ_0 m.H; E/V = -μ_0Μ.Η

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Τοrque from the Zeeman energy

τ = μ_0 H x m = μ_0 H m sin(θ)

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How can a magnet respond to a magnetic field

align its body or align its magnetism (focus on this one)

5
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Magnetism rotation

large volume of magnetisation coherently changes direction (happens when switching along a hard axis); as H decreases anisotropy dominates and magnetisation rotates towards easy axis; reversibly follows energy minimum

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Anisotropy field

magnetic field of equilavent strength to the influence of anisotropy (where the hysterisis curve flattens in hard axis); Hk = -2K/(μ_0 Ms)

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Domain nucleation

magnetism doesn’t rotate gradually in most cases but changes abruptly; reverse domain suddenly nucleates at a critical field strength and begins to grow; irreversible, sudden change; occurs at weak points in the magnetisation structure eg edges (strongest demag field) or defects

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Domain wall motion

Nucleated domain walls can move, flipping adjacent domains to align with it

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What is Barkhaussen noise

changing magnetic flux induces a voltage/current which can be amplified through a speaker producing a hissing noise; shows the material is changing via a large number of small steps rather than perfectly smoothly

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What causes these small steps

domain walls become pinned against non magnetic defects and form stable closed flux domains; this is an energy barrier against domain wall motion; field increases until enough energy to ping off defect and form full domain

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<p>Describe how magnetisation is changing in this hysterisis loop</p>

Describe how magnetisation is changing in this hysterisis loop

1) moments mostly saturated, small relaxation by rotation;

2) Nucleation of reverse domains due to demag and applied field;

3) Irreversible domain wall motion, bulk of reversal process;

4) small magnetisation rotation to be fully saturated

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Magnetisation reversal along the hard axis

reversal via gradual rotation of magnetisation, no metastable states to go through as always fighting the anisotropy energy; produces linear reversible hysterisis plot