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MAGNETIC METALS STRUCTURE –PROPERTIES APPLICATIONS Howard H. Liebermann, Ph.D.

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Page 1: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

MAGNETIC METALSSTRUCTURE –PROPERTIES

APPLICATIONS

Howard H. Liebermann, Ph.D.

Page 2: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Fundamentals

Structure of Metals On atomic level, regular arrangement of atoms immersed

in “sea” of “free electrons”. Results of this:

Metallic bond Electrical, thermal conductivity Ductility

Typical arrangements of atoms: BCC, FCC, HCP

Atypical arrangement of atoms: Amorphous

H.H. Liebermann 2

Page 3: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Cubic Crystal Systems

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FCCBCCSimple Cube

Page 4: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Basic Magnetics

Electron has negative charge Orbiting of electrons about atom induces magnetic

moment (vector) These magnet moments can interact

with one another with an external applied magnetic field

Extent of interaction determines what kind of magnetism (exchange vs. anisotropy)

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Page 5: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetic Axes in BCC (Fe)

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Page 6: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetic Axes in FCC (Ni)

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Page 7: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Kinds of Magnetism

Ferromagnetism: magnetic spin interaction is large – applied external magnetic field doesn’t affect this

Paramagnetism: magnetic spins tend to align in the direction of applied field

Diamagnetism: magnetic spins tend to align in the direction away from applied field

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Page 8: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Some Magnetic Characteristics

Exchange - strong interaction between magnetization vectors

Anisotropy – preferential direction for magnetization vector in a material

Magnetostriction – interaction between stress (applied, residual, etc.) and magnetization vector direction

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Page 9: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Curie Temperature

Temperature above which sample magnetization ceases.

True for ferromagnetic, paramagnetic, etc. Potential in sensor applications.

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Page 10: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Exchange Interaction

Quantum mechanical effect:

Tendency for adjacent magnetic vectors to align directionally.

Affected by thermal energy.

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Page 11: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetic Anisotropy

Origin: Tropy – direction Iso – constant An – not

Conclusion – not constant with direction in an alloy.

Magnetic anisotropy result of: Crystal structure of alloy. Shape of sample being tested. Magnetic field induced.

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Page 12: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetostriction

Link between change in magnetic sample dimensions (stress) and applied magnetic field.

Reciprocity abounds.

Stress can result from numerous causes: Forces applied to magnetic sample. Residual forces resulting from cooling on heat treating. Forces arising during use of a device.

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Page 13: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Schematic Example

Iron

Cobalt

Iron + Cobalt

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Page 14: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetic Domain Wall Width

w ~

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εK

Page 15: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetization Loop

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Page 16: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Magnetic Domain Wall Motion

No external field (applied, residual, etc.) and magnetization vector direction

Low external field

High external field

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Page 17: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Other Domain Wall Mechanisms

Rotational

Reverse domain nucleation

Eddy current generation Magnetic losses Electrical losses Heat losses

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Page 18: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Hard vs. Soft Magnets

Hard Soft

• robust magnetic field • easily demagnetized

• largely impervious to external fields

• high permeability

• can be costly • switching applications

• provide strong field

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Page 19: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Applications of Magnetic Mat’ls

Hard Soft• stators/rotors • low loss transformers• motors/generators • inductors (various)

• EAS (bias alloy) • Invar (Fe-Ni) alloys• refridge door gaskets, etc. • nanocrystalline• toys • Maglev train

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Page 20: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Applications of Hard Magnets

Field of Application

Products Requirements Materials

• Permanent Magnets

• Loudspeakers• Small

generators/motors• Sensors

• Large H C and MR • Fe-based• Fe+ ~(0.7–5)% Si• Fe +~(35-50)%Co

• Analog Data Storage

• Video tape• Audio tape

• Medium H C and MR (hysteresis loop square)

• Fe/Co/Ni/Al/Cu = 50/24/14/9/3

• SmCo5

• Sm2Co17

• Nd2Fe14B

• Digital Data Storage

• Hard, floppy disc• Bubble memory

• Special magnetic domain structure

• NiCo, NiCoFe• CrO2

• Fe2O3

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Page 21: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Field of Application Products Requirements Materials

• Analog Data Storage

• Video tape• Audio tape

• Medium H C and MR (square hysteresis loop)

• Fe/Co/Ni/Al/Cu = 50/24/14/9/3

• SmCo5

• Sm2Co17

• Nd2Fe14B

• Digital Data Storage

• Hard, floppy disc

• Bubble memory

• Special magnetic domain structure

• Ni/Co, Ni/Co/Fe• CrO2

• Fe2O3

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Applications of Hard Magnets

Page 22: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Field of Application Products Requirements Materials

• Power Conversion• Motors• Generators• Electromagnets

• Large MR

• Small Hc

• Losses low

• Fe-based• Fe+ ~(0.7–5)% Si• Fe +~(35-50)%Co

• Power Adaptation • Power Transformers

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Applications of Soft Magnets

Page 23: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Field of Application Products Requirements Materials

• Signal Transfer

• Other Transformers • Linear M-H

curve

• LF (<100kHz) • Low conductivity

• Fe+36%Fe/Ni/Co = 20/40/40

• HF (>100kHz) • Very low conductivity

• Ni–Zn ferrites

• Magnetic Shielding/EAS

• Permalloy• Mu metal

• Large dM/dH @ H=0

• Ni/Fe/Cu/Cr ~77/16/5/2

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Applications of Soft Magnets

Page 24: Howard H. Liebermann, Ph.D..  Structure of Metals  On atomic level, regular arrangement of atoms immersed in “sea” of “free electrons”.  Results of

Summary

Wide variety of materials/applications. Elementary concepts of materials science as they

apply to magnetic materials. Aspects of alloy design (chemistry) and resulting

effects on magnetic properties.

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