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Magnetic Materials
Properties of
antiferromagneticmaterials
The spin alignment is in antiparallel manner.
Properties of
antiferromagneticmaterials
The spin alignment is in antiparallel manner.
So net magnetic moment is zero.
Properties of
antiferromagneticmaterials
The spin alignment is in antiparallel manner.
So net magnetic moment is zero.
Susceptibility is small and positive.
Properties of
antiferromagneticmaterials
The spin alignment is in antiparallel manner.
So net magnetic moment is zero.
Susceptibility is small and positive.
Initially susceptibility increases with increase in
temperature and beyond Neel temperature the
susceptibility decreases with temperature.
Properties of
antiferromagneticmaterials
The spin alignment is in antiparallel manner.
So net magnetic moment is zero.
Susceptibility is small and positive.
Initially susceptibility increases with increase in
temperature and beyond Neel temperature the
susceptibility decreases with temperature.
At Neel temperature susceptibility is maximum.
Examples: FeO, MnO, Cr2O3 and salts of
transition elements.
Properties of ferrimagnetic
materials
Special type of antiferromagnetic material.
Properties of ferrimagnetic
materials
Special type of antiferromagnetic material.
The spin alignment is antiparallel but different
magnitude.
Properties of ferrimagnetic
materials
Special type of antiferromagnetic material.
The spin alignment is antiparallel but different
magnitude.
So they possess net magnetic moment.
Also called ferrites.
Properties of ferrimagnetic
materials
Special type of antiferromagnetic material.
The spin alignment is antiparallel but different
magnitude.
So they possess net magnetic moment.
Also called ferrites.
Susceptibility is very large and positive.
Examples: ferrous ferrite, nickle ferrite
Domain Theory of
Ferromagnetic Materials
Domain Theory of Ferromagnetic Materials
Materials that retain a
magnetization in
zero field
Domain Theory of Ferromagnetic Materials
Materials that retain a
magnetization in
zero field
Quantum mechanical
exchange
Domain Theory of Ferromagnetic Materials
Materials that retain a
magnetization in
zero field
Quantum mechanical
exchange
interactions favour parallel
alignment of moments
Domain Theory of Ferromagnetic Materials
Materials that retain a
magnetization in
zero field
Quantum mechanical
exchange
interactions favour parallel
alignment of moments
Examples: iron, cobalt
Domain Theory of Ferromagnetic Materials
Ferromagnetic
materials tend to form
magnetic domains
Domain Theory of Ferromagnetic Materials
Ferromagnetic
materials tend to form
magnetic domains
Each domain is
magnetized in a
different direction
Domain Theory of Ferromagnetic Materials
Ferromagnetic
materials tend to form
magnetic domains
Each domain is
magnetized in a
different direction
Domain structure
minimizes energy due
to stray fields
Domain Theory of Ferromagnetic Materials
Applying a field changes
domain structure
Domain Theory of Ferromagnetic Materials
Applying a field changes
domain structure
Domains with
magnetization in
direction of field grow
Domain Theory of Ferromagnetic Materials
Applying a field changes
domain structure
Domains with
magnetization in
direction of field grow
Other domains shrink
Two ways for aligning of magnetic domains:
1.Growth of favorably oriented domains (initially)
2.Rotation of domains (finally)
Applying very strong fields can saturate
magnetization by creating single domain
Domain Theory of Ferromagnetic Materials
Domain Theory of Ferromagnetic Materials
Hysteresis, Remanence, & Coercivity of Ferromagnetic Materials
Domain Theory of Ferromagnetic Materials
“hard” ferromagnetic material
has a large M0 and large Hc.
“soft” ferromagnetic material
has both a small M0 and Hc.
Domain Theory of Ferromagnetic Materials
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Coercivity & Retentivity are large Coercivity & Retentivity are small.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Coercivity & Retentivity are large Coercivity & Retentivity are small.
Cannot be easily magnetized &
demagnetized
Can be easily magnetized &
demagnetized.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Coercivity & Retentivity are large Coercivity & Retentivity are small.
Cannot be easily magnetized &
demagnetized
Can be easily magnetized &
demagnetized.
Magneto static energy is large. Magneto static energy is small.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Coercivity & Retentivity are large Coercivity & Retentivity are small.
Cannot be easily magnetized &
demagnetized
Can be easily magnetized &
demagnetized.
Magneto static energy is large. Magneto static energy is small.
Have small values of permeability and
susceptibility
Have large values of susceptibility and
permeability.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Coercivity & Retentivity are large Coercivity & Retentivity are small.
Cannot be easily magnetized &
demagnetized
Can be easily magnetized &
demagnetized.
Magneto static energy is large. Magneto static energy is small.
Have small values of permeability and
susceptibility
Have large values of susceptibility and
permeability.
Used to make permanent magnets. Used to make electromagnets.
Hard and Soft Magnetic
materials
Hard Magnetic Material Soft Magnetic Material
Have large hysteresis loss. Have low hysteresis loss.
Domain wall moment is difficult Domain wall moment is relatively
easier.
Coercivity & Retentivity are large Coercivity & Retentivity are small.
Cannot be easily magnetized &
demagnetized
Can be easily magnetized &
demagnetized.
Magneto static energy is large. Magneto static energy is small.
Have small values of permeability and
susceptibility
Have large values of susceptibility and
permeability.
Used to make permanent magnets. Used to make electromagnets.
Iron-nickel-aluminum alloys, copper-
nickle-iron alloys, copper–nickel–
cobalt alloys
Iron- silicon alloys, ferrous- nickel
alloys, ferrites, garnets.

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magnetic Hystersis magnetic Hystersis magnetic Hystersis magnetic Hystersis

  • 2. Properties of antiferromagneticmaterials The spin alignment is in antiparallel manner.
  • 3. Properties of antiferromagneticmaterials The spin alignment is in antiparallel manner. So net magnetic moment is zero.
  • 4. Properties of antiferromagneticmaterials The spin alignment is in antiparallel manner. So net magnetic moment is zero. Susceptibility is small and positive.
  • 5. Properties of antiferromagneticmaterials The spin alignment is in antiparallel manner. So net magnetic moment is zero. Susceptibility is small and positive. Initially susceptibility increases with increase in temperature and beyond Neel temperature the susceptibility decreases with temperature.
  • 6. Properties of antiferromagneticmaterials The spin alignment is in antiparallel manner. So net magnetic moment is zero. Susceptibility is small and positive. Initially susceptibility increases with increase in temperature and beyond Neel temperature the susceptibility decreases with temperature. At Neel temperature susceptibility is maximum. Examples: FeO, MnO, Cr2O3 and salts of transition elements.
  • 7. Properties of ferrimagnetic materials Special type of antiferromagnetic material.
  • 8. Properties of ferrimagnetic materials Special type of antiferromagnetic material. The spin alignment is antiparallel but different magnitude.
  • 9. Properties of ferrimagnetic materials Special type of antiferromagnetic material. The spin alignment is antiparallel but different magnitude. So they possess net magnetic moment. Also called ferrites.
  • 10. Properties of ferrimagnetic materials Special type of antiferromagnetic material. The spin alignment is antiparallel but different magnitude. So they possess net magnetic moment. Also called ferrites. Susceptibility is very large and positive. Examples: ferrous ferrite, nickle ferrite
  • 12. Domain Theory of Ferromagnetic Materials Materials that retain a magnetization in zero field
  • 13. Domain Theory of Ferromagnetic Materials Materials that retain a magnetization in zero field Quantum mechanical exchange
  • 14. Domain Theory of Ferromagnetic Materials Materials that retain a magnetization in zero field Quantum mechanical exchange interactions favour parallel alignment of moments
  • 15. Domain Theory of Ferromagnetic Materials Materials that retain a magnetization in zero field Quantum mechanical exchange interactions favour parallel alignment of moments Examples: iron, cobalt
  • 16. Domain Theory of Ferromagnetic Materials Ferromagnetic materials tend to form magnetic domains
  • 17. Domain Theory of Ferromagnetic Materials Ferromagnetic materials tend to form magnetic domains Each domain is magnetized in a different direction
  • 18. Domain Theory of Ferromagnetic Materials Ferromagnetic materials tend to form magnetic domains Each domain is magnetized in a different direction Domain structure minimizes energy due to stray fields
  • 19. Domain Theory of Ferromagnetic Materials Applying a field changes domain structure
  • 20. Domain Theory of Ferromagnetic Materials Applying a field changes domain structure Domains with magnetization in direction of field grow
  • 21. Domain Theory of Ferromagnetic Materials Applying a field changes domain structure Domains with magnetization in direction of field grow Other domains shrink
  • 22. Two ways for aligning of magnetic domains: 1.Growth of favorably oriented domains (initially) 2.Rotation of domains (finally) Applying very strong fields can saturate magnetization by creating single domain Domain Theory of Ferromagnetic Materials
  • 23. Domain Theory of Ferromagnetic Materials
  • 24. Hysteresis, Remanence, & Coercivity of Ferromagnetic Materials Domain Theory of Ferromagnetic Materials
  • 25. “hard” ferromagnetic material has a large M0 and large Hc. “soft” ferromagnetic material has both a small M0 and Hc. Domain Theory of Ferromagnetic Materials
  • 26. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss.
  • 27. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier.
  • 28. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier. Coercivity & Retentivity are large Coercivity & Retentivity are small.
  • 29. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier. Coercivity & Retentivity are large Coercivity & Retentivity are small. Cannot be easily magnetized & demagnetized Can be easily magnetized & demagnetized.
  • 30. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier. Coercivity & Retentivity are large Coercivity & Retentivity are small. Cannot be easily magnetized & demagnetized Can be easily magnetized & demagnetized. Magneto static energy is large. Magneto static energy is small.
  • 31. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier. Coercivity & Retentivity are large Coercivity & Retentivity are small. Cannot be easily magnetized & demagnetized Can be easily magnetized & demagnetized. Magneto static energy is large. Magneto static energy is small. Have small values of permeability and susceptibility Have large values of susceptibility and permeability.
  • 32. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier. Coercivity & Retentivity are large Coercivity & Retentivity are small. Cannot be easily magnetized & demagnetized Can be easily magnetized & demagnetized. Magneto static energy is large. Magneto static energy is small. Have small values of permeability and susceptibility Have large values of susceptibility and permeability. Used to make permanent magnets. Used to make electromagnets.
  • 33. Hard and Soft Magnetic materials Hard Magnetic Material Soft Magnetic Material Have large hysteresis loss. Have low hysteresis loss. Domain wall moment is difficult Domain wall moment is relatively easier. Coercivity & Retentivity are large Coercivity & Retentivity are small. Cannot be easily magnetized & demagnetized Can be easily magnetized & demagnetized. Magneto static energy is large. Magneto static energy is small. Have small values of permeability and susceptibility Have large values of susceptibility and permeability. Used to make permanent magnets. Used to make electromagnets. Iron-nickel-aluminum alloys, copper- nickle-iron alloys, copper–nickel– cobalt alloys Iron- silicon alloys, ferrous- nickel alloys, ferrites, garnets.