Magnetic Materials
Magnetic materials respond to applied fields through orbital and spin magnetic moments. The magnetization $\vec M$ creates bound currents that modify the field. The auxiliary field $\vec H$ plays the same role for magnetostatics that $\vec D$ plays for electrostatics — it satisfies Ampere's law with only free currents.
Key Concepts
Key Equations
H and B in a Magnetic Material
A solenoid ( turns/m, A) has an iron core with . Find and inside.
A/m.
Exercises
7 problemsA solenoid ( turns/m, A) in air. Find inside (in A/m).
Same solenoid but with iron core (). Find inside (in T).
For a paramagnetic material with , find .
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Upgrade to Pro →A magnetic material has T and . Find (in A/m).
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Upgrade to Pro →Same material. Find (in A/m) if (so ).
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Upgrade to Pro →Energy density in a magnetic field: . For T, (in J/m³).
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Upgrade to Pro →Magnetic field of a diamagnetic sphere in external field : . For (diamagnet) and A/m, find (in A/m).
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Upgrade to Pro →Key Takeaways
- satisfies Ampere's law for free currents; includes all (free and bound) currents.
- Linear media: , (paramagnets), (diamagnets), (ferromagnets).
- Bound surface and volume currents from are the magnetic analogs of bound charges from .
- Ferromagnet hysteresis: irreversible magnetization — the basis of permanent magnets and magnetic memory.