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Insulated Powder Composites Brochure.QXD (Page 3) - GKN

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HOEGANAES<br />

INSULATED POWDER COMPOSITES<br />

CHARACTERISTICS AND ELECTROMAGNETIC<br />

APPLICATION GUIDELINES


HOEGANAES<br />

INSULATED POWDER COMPOSITES<br />

INTRODUCTION<br />

The molecular field theory was developed nearly<br />

100 years ago. At that time, it was explained that<br />

groups of iron atoms are magnetized in one<br />

direction with equal groups of atoms magnetized<br />

in the opposite direction, thus fully compensating<br />

each other with zero net magnetic moment.<br />

These groups of atoms are referred to as<br />

magnetic domains. In a given iron powder<br />

particle, there are a substantial number of<br />

domains all arranged in a way to give a zero<br />

magnetic moment. Extremely fine particles can<br />

potentially represent single domain structures.<br />

Lodestone happens to be a natural, single domain<br />

iron ore (magnetite), which exhibits intrinsic<br />

permanent magnet characteristics. Its discovery<br />

had a significant impact on the history of the<br />

world. The development of <strong>Insulated</strong> <strong>Powder</strong><br />

<strong>Composites</strong> represents the next step toward<br />

further advancement in soft magnetic material<br />

systems!<br />

BENEFITS OF THE POWDER<br />

METALLURGY PROCESS<br />

• Net Shape Capability<br />

• Complex Shapes<br />

• Engineered Materials<br />

• High Production Rates<br />

• Tolerance Control<br />

• Good Surface Finish<br />

BENEFITS OF INSULATED<br />

POWDER MATERIALS<br />

• Isotropic magnetic structure permits<br />

3-dimensional magnetic<br />

flux path capability<br />

• Easily shaped into complex<br />

configurations using<br />

conventional powder<br />

metallurgy compaction<br />

process<br />

• Similar magnetic saturation<br />

induction values to wrought<br />

steel laminations<br />

• Low inherent eddy current<br />

losses associated with the<br />

dielectric polymer coating<br />

• Flexibility to engineer<br />

performance characteristics<br />

to satisfy application<br />

requirements<br />

• Preferred alternative to<br />

laminations for new electric<br />

motor designs


APPLICATIONS CHART<br />

For switching actuators and ignition coils, fuel injectors,<br />

motor applications<br />

Resistivity Strength Induction B Permeability<br />

microohm-meter<br />

(MPa) 10 kA/m (T) Max<br />

Ancorlam >50 90 1.47 470<br />

Ancorlam HR >1300 60 1.52 400<br />

Ancorlam 2HR* >475 90 1.64 610<br />

For higher frequency applications, power electronics<br />

Resistivity Strength Induction B Permeability<br />

microohm-meter<br />

(MPa) 10 kA/m (T) Max<br />

Ancorlam 2FHR >1300 60 1.51 360<br />

Ancorlam HR >1300 60 1.51 400<br />

For motor applications requiring high induction and<br />

permeability, actuators, frequencies up to 400 Hz<br />

Resistivity Strength Induction B Permeability<br />

microohm-meter<br />

(MPa) 10 kA/m (T) Max<br />

Ancorlam 2 50 50 1.60 550<br />

Ancorlam 2HR* 475 90 1.64 610<br />

*Density of 7.6 g/cm 3<br />

Grade modification is possible to meet application<br />

specific properties<br />

CONVERSIONS / CALCULATIONS<br />

1 Tesla = Gauss X 10 -4<br />

1 Tesla = 1 Weber per meter 2<br />

1 Gauss = 1 Maxwell per cm 2<br />

Amp-Turns per meter = Oersteds x 79.5 (1 Amp-Turn per meter = 0.0125 Oe)<br />

Tesla/Meter = Gauss x 1.26 10 -6<br />

Amp-Turns Oersted<br />

Frequency =<br />

rpm x Number of Poles (rotating electrical devices)<br />

120<br />

Inductance = L = 4πµA<br />

N 2 I<br />

L = Inductance (mH)<br />

µ = Permeability<br />

A = Cross-sectional area (cm 2 )<br />

I = Path length (cm)<br />

N = Number of turns<br />

POWDER METALLURGY<br />

PROCESSES FOR<br />

ELECTROMAGNETIC GRADES<br />

Composite Production:<br />

Admix Metal <strong>Powder</strong>, Additives,<br />

Coating Materials<br />

Press Ready<br />

<strong>Insulated</strong> <strong>Powder</strong> Composite<br />

Material<br />

Cold or Warm Compaction<br />

Optional<br />

Secondary Curing or Stress<br />

Relieving<br />

Optional Finishing Processes:<br />

Machining<br />

Polymer Impregnation<br />

Plating<br />

Finished Electromagnetic<br />

Component<br />

100µm<br />

Microstructure illustrating insulative coating


HOEGANAES<br />

INSULATED POWDER COMPOSITES<br />

Iron powders exposed to a magnetic field<br />

gradually begin to realign the individual<br />

domains by slowly orienting themselves toward<br />

the direction of the applied magnetic field.<br />

When the magnetic field is switched off, the<br />

domains remain partially oriented in the original<br />

magnetic direction. Zero magnetism is realized<br />

when the reverse field equals the coercive<br />

force. With further increases in the reverse field,<br />

the domains revert to the new direction.<br />

The field required to reverse the domain<br />

depends upon the crystalline symmetry and<br />

anisotropic properties. This energy is very small<br />

in the case of a soft magnetic material, and<br />

considerably greater for a hard magnetic<br />

material, i.e., types that maintain high<br />

remanence, typically referred to as permanent<br />

magnets.<br />

The most commonly used soft magnetic<br />

material involves electrical steel laminations for<br />

low frequency (60 – 200 Hz) applications.<br />

Low-end performance materials include<br />

cold-rolled, motor lamination steels, whereas<br />

intermediate to high-end characteristics are<br />

achieved with silicon-iron, or oriented steels.<br />

Laminations are prevalent because of existing<br />

design familiarity, relatively low costs and<br />

adequate magnetic performance. Nevertheless,<br />

the limited two-dimensional flux path capability<br />

and relatively low energy efficiency at higher<br />

operating frequency make them undesirable for<br />

new electric motor designs.<br />

INSULATED POWDER COMPOSITES<br />

The introduction of uniformly coated iron<br />

particles providing a three-dimensional<br />

distributed air gap with an isotropic flux path,<br />

allows designers to reconsider conventional<br />

topology restrictions typical of steel<br />

laminations. Along with the benefits of PM net<br />

shape manufacturing capability, insulated<br />

composite materials exhibit inherently low<br />

eddy current losses even when subjected to<br />

operating frequencies exceeding 400 Hz.<br />

Composite manufacturing flexibility provides<br />

the ability to engineer soft magnetic<br />

characteristics to suit specific application<br />

requirements. Incorporating different iron<br />

powder size distributions, and coating types to<br />

increase resistivity, various attributes can be<br />

manipulated to enhance the material’s<br />

permeability, structural density or core-loss<br />

characteristics.<br />

Coupling new electrical device design<br />

topologies with insulated powder composites<br />

and high-energy permanent magnets provides<br />

the necessary performance enhancements<br />

along with concurrent improvements in<br />

component efficiency, packaging and simplified<br />

manufacturing processes. The additional<br />

magnetizing force (mmf) of the permanent<br />

magnet compensates for the lower permeability<br />

of the soft magnetic composite grades.<br />

The complementary materials and new designs<br />

provide greater performance and enhanced<br />

efficiency, with the ability to reduce<br />

manufacturing costs and component<br />

package size.<br />

Applications for these magnetic materials<br />

include high-efficiency electric motors,<br />

high-frequency transformers, and unique<br />

electrical components. The electrical design<br />

engineer has three-dimensional shape-making<br />

flexibility plus the high material utilization<br />

inherent with the PM process. Design flexibility<br />

is enhanced further by the ability to bond<br />

together small segments to form larger, more<br />

complex shapes.


INSULATED POWDER COMPOSITE PERFORMANCE<br />

AncorLam<br />

AncorLam HR<br />

AncorLam 2F HR<br />

Compacting pressure (MPa) 830 830 830 830 830<br />

<strong>Powder</strong> temp. ( o C) RT RT RT RT RT<br />

Tool temp. ( o C) 80 80 80 80 80<br />

Curing temp. ( o C) >300 >300 >300 >300 >300<br />

Cured density 7.47 7.45 7.6 7.43 7.5<br />

Induction B @ 10 kA/m (T) 1.47 1.52 1.64 1.5 1.6<br />

Permeability at 60 Hz 470 370 610 360 550<br />

Resistivity, micro-ohm-meter >50 >1300 >500 >1300 >50<br />

Coercive field strength (A/m) 300 270 246 280 245<br />

Strength (MPa) 90 60 90 60 40<br />

Core-loss @ 1T (watts/kg)<br />

AncorLam 2 HR<br />

60 Hz 9 7.6 6.6 7.3 9<br />

100 Hz 15 13 11.2 13.5 15<br />

200 Hz 31 27 24 27 31<br />

400 Hz 67 53 52 54 67<br />

1000 Hz - 147 172 146 245<br />

AncorLam 2<br />

All properties improve with higher compaction pressures(density), especially induction, permeability and core-loss.<br />

<strong>Insulated</strong> <strong>Powder</strong> Composite manufacturing flexibility provides the ability to engineer soft<br />

magnetic characteristics to suit specific application requirements. Incorporating different iron<br />

powder size distributions and coating types to increase bulk resistivity various attributes can be<br />

manipulated to enhance the material’s structural density, induction, permeability or core-loss<br />

characteristics.<br />

Grade modification is possible to meet application specific properties.


AncorLam ®<br />

Induction in Tesla<br />

AncorLam ® is a high performance insulated powder material suitable for a variety of soft magnetic<br />

applications. Specific applications include switching actuators and ignition coils, fuel injectors, and<br />

motor applications.<br />

AncorLam ® consists of high purity iron powder with a specialized coating/lubricant system that<br />

minimizes hysteresis and eddy current losses over a range of frequencies. This material is provided<br />

as a press-ready premix for warm or cold die compaction.<br />

AncorLam is a lower cost option giving good balance between Core Loss and Induction.<br />

Performance of AncorLam ® at 7.45 g/cm 3<br />

Induction at 40 kA/m (T) 1.90<br />

Induction at 10 kA/m (T) 1.47<br />

Maximum permeability 470<br />

Coercive field strength (A/m) 300<br />

Core-loss at 400 Hz, 1T, W/kg 67<br />

Core-loss 1 kHz, 1T, W/kg —<br />

Green density (g/cm3 ) 7.47<br />

Cured strength (MPa) 90<br />

Resistivity micro-ohm-meter >50<br />

Apparent density (g/cm3 ) 2.85-3.10<br />

Hall flow (s/50 g) 32 max<br />

HYSTERESIS LOOP<br />

AncorLam<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

-5000 -4000 -3000 -2000 -1000 0 1000 2000 3000 4000 5000<br />

-0.5<br />

-1<br />

-1.5<br />

-2<br />

-2.5<br />

Applied Field in A/m


AncorLam ® (continued)<br />

Core-loss in Watts/kg<br />

Core-loss in Watts/kg<br />

10000<br />

1000<br />

100<br />

0.1<br />

0.01<br />

500<br />

450<br />

400<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

10<br />

1<br />

CORE-LOSS VS. INDUCTION<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1k Hz, 5k Hz, 10 kHz<br />

0.001<br />

0.001 0.01 0.1<br />

Induction in Tesla<br />

1 10<br />

PERMEABILITY VS. INDUCTION, FREQUENCY<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz<br />

5000 Hz<br />

10 kHz<br />

0<br />

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2<br />

60 Hz<br />

Induction in Tesla<br />

60 Hz<br />

10 kHz<br />

5 kHz<br />

1 kHz<br />

400 Hz<br />

200 Hz<br />

100 Hz<br />

60 Hz


AncorLam ® HR<br />

Induction in Tesla<br />

AncorLam ® HR has a constant permeability over a wide frequency range providing a lower cost<br />

option for high frequency applications.<br />

AncorLam ® HR consists of high purity iron powder with a specialized coating/lubricant system that<br />

minimizes hysteresis and eddy current losses over a range of frequencies. This material is provided<br />

as a press ready premix for warm or cold die compaction.<br />

Performance of AncorLam ® HR at 7.45 g/cm 3<br />

Induction at 40 kA/m (T) 1.90<br />

Induction at 10 kA/m (T) 1.52<br />

Maximum permeability 370<br />

Coercive field strength (A/m) 270<br />

Core-loss at 400 Hz, 1T, W/kg 53<br />

Core-loss 1 kHz, 1T, W/kg 147<br />

Green density (g/cm3 ) 7.45<br />

Cured strength (MPa) 60<br />

Resistivity micro-ohm-meter >1300<br />

Apparent density (g/cm3 ) 2.85-3.10<br />

Hall flow (s/50 g) 32 max<br />

HYSTERESIS LOOP<br />

AncorLam HR<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

-5000 -4000 -3000 -2000 -1000 0 1000 2000 3000 4000 5000<br />

-0.5<br />

-1<br />

-1.5<br />

-2<br />

-2.5<br />

Applied Field in A/m


AncorLam ® HR (continued)<br />

Core-loss in Watts/kg<br />

Permeability<br />

10000<br />

1000<br />

400<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

100<br />

0<br />

10<br />

0.0001<br />

1<br />

0.1<br />

0.01<br />

0.001<br />

CORE-LOSS AT VARIOUS FREQUENCIES AND INDUCTION<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

0.001 0.01 0.1 1 10<br />

PERMEABILITY AT VARIOUS FREQUENCIES<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

10000 Hz<br />

Induction in Tesla<br />

0 0.4 0.8 1.2 1.6 2<br />

Induction in Tesla<br />

60 Hz<br />

10 kHz<br />

5 kHz<br />

1 kHz<br />

400 Hz<br />

200 Hz<br />

100 Hz<br />

60 Hz


AncorLam ® 2HR<br />

Induction in Tesla<br />

AncorLam ® 2 HR is bested suited for motor and actuator applications. Providing good induction and<br />

permeability for applications up to 1000 HZ.<br />

AncorLam ® 2 HR consists of high purity iron powder with a specialized coating/lubricant system that<br />

increase permeability while limiting losses. This material is provided as a press ready premix for<br />

warm or cold die compaction.<br />

Performance of AncorLam ® 2HR<br />

Induction at 40 kA/m (T) 2.02*<br />

Induction at 10 kA/m (T) 1.64*<br />

Maximum permeability 610*<br />

Coercive field strength (A/m) 246*<br />

Core-loss at 400 Hz, 1T, W/kg 52*<br />

Core-loss 1 kHz, 1T, W/kg 172*<br />

Green density (g/cm3 ) 7.60*<br />

Cured strength (MPa) 90*<br />

Resistivity micro-ohm-meter >475*<br />

Apparent density (g/cm3 ) 2.85-3.10*<br />

Hall flow (s/50 g)<br />

* Density is 7.6 g.cm<br />

32 max*<br />

3<br />

HYSTERESIS LOOP<br />

AncorLam 2HR*(7.6 DENSITY)<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

-10000 -8000 -6000 -4000 -2000 0 2000 4000 6000 8000 10000<br />

-0.5<br />

-1<br />

-1.5<br />

-2<br />

-2.5<br />

Applied Field in A/m


AncorLam ® 2HR (continued)<br />

Core-loss in Watts/kg<br />

Permeability<br />

10000<br />

1000<br />

100<br />

10<br />

1<br />

0.1<br />

0.01<br />

0.001<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

0<br />

CORE-LOSS VS INDUCTION (7.6 DENSITY)<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

0.0001<br />

0.01 0.1 1 10<br />

Induction in Tesla<br />

PERMEABILITY VS INDUCTION (7.6 DENSITY)<br />

60 Hz, 100 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

60 Hz<br />

10 kHz<br />

0 0.5 1 1.5 2 2.5<br />

Induction in Tesla<br />

10 kHz<br />

5 kHz<br />

1 kHz<br />

400 Hz<br />

200 Hz<br />

100 Hz<br />

60 Hz


AncorLam ® 2FHR<br />

Induction in Tesla<br />

AncorLam ® 2FHR is targeted and engineered for higher frequency applications up to 31 Khz.<br />

AncorLam ® 2FHR consists of high purity iron powder with a specialized coating/lubricant system that<br />

minimizes hysteresis and eddy current losses over a range of frequencies. This material is provided<br />

as a press ready premix for warm or cold die compaction.<br />

Performance of Ancorlam ® 2FHR at 7.45 g/cm 3<br />

Induction at 40 kA/m (T) 1.90<br />

Induction at 10 kA/m (T) 1.50<br />

Maximum permeability 360<br />

Coercive field strength (A/m) 300<br />

Core-loss at 400Hz, 1T, W/kg 54<br />

Core-loss 1kHz, 1T, W/kg 146<br />

Green density (g/cm3 ) 7.43<br />

Cured strength (MPa) 60<br />

Resistivity micro-ohm-meter >1300<br />

Apparent density (g/cm3 ) 2.85-3.10<br />

Hall flow (s/50 g) 32 max<br />

HYSTERESIS LOOP<br />

AncorLam 2FHR<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

-5000 -4000 -3000 -2000 -1000 0 1000 2000 3000 4000 5000<br />

-0.5<br />

-1<br />

-1.5<br />

-2<br />

-2.5<br />

Applied Field in A/m


AncorLam ® 2FHR (continued)<br />

Core-loss in Watts/kg<br />

Permeability<br />

10000<br />

1000<br />

100<br />

10<br />

1<br />

0.1<br />

0.01<br />

400<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

CORE-LOSS AT VARIOUS FREQUENCIES<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

0.001<br />

0.001 0.01 0.1 1 10<br />

PERMEABILITY AT VARIOUS FREQUENCIES AND INDUCTION<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

10000 Hz<br />

Induction in Tesla<br />

0 0.4 0.8 1.2 1.6 2<br />

Induction in Tesla<br />

60 Hz<br />

10 kHz<br />

5 kHz<br />

1 kHz<br />

400 Hz<br />

200 Hz<br />

100 Hz<br />

60 Hz


AncorLam ® 2<br />

AncorLam ® 2 is a high performance insulated powder material suitable for a variety of soft magnetic<br />

applications that require high permeability. Used for applications up to 400 HZ.<br />

Performance of AncorLam ® 2 at 7.45 g/cm 3<br />

Induction at 40 kA/m (T) 1.95<br />

Induction at 10 kA/m (T) 1.60<br />

Maximum permeability 550<br />

Coercive field strength (A/m) 245<br />

Core-loss at 400 Hz, 1T, W/kg 67<br />

Core-loss 1 kHz, 1T, W/kg 245<br />

Green density (g/cm3 ) 7.49<br />

Cured strength (MPa) 40<br />

Resistivity micro-ohm-meter >50<br />

Apparent density (g/cm3 ) 2.85-3.10<br />

Hall flow (s/50 g) 32 max<br />

Induction in Tesla<br />

DC HYSTERESIS LOOP<br />

AncorLam 2<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

-5000 -4000 -3000 -2000 -1000 0 1000 2000 3000 4000 5000<br />

-0.5<br />

-1<br />

-1.5<br />

Applied Field in A/m<br />

-2<br />

-2.5<br />

Applied Field in A/m


AncorLam ® 2 (continued)<br />

Core-loss in Watts/kg<br />

Permeability<br />

10000<br />

1000<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

100<br />

10<br />

1<br />

0.1<br />

0.01<br />

CORE-LOSS AT VARIOUS FREQUENCIES<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

0.001<br />

0.001 0.01 0.1 1 10<br />

AC PERMEABILITY<br />

60 Hz, 100 Hz, 200 Hz, 400 Hz, 1000 Hz, 5000 Hz, 10000 Hz<br />

10000 Hz<br />

Induction in Tesla<br />

0<br />

0 0.5 1 1.5 2 2.5<br />

60 Hz<br />

Induction in Tesla<br />

10 kHz<br />

5 kHz<br />

1 kHz<br />

400 Hz<br />

200 Hz<br />

100 Hz<br />

60 Hz


RELEVANCE OF MATERIAL CHARACTERISTICS ON END-USE<br />

PERFORMANCE FOR ELECTROMAGNETIC DEVICES<br />

Permeability Influences the output power of<br />

the electrical device. Wrought lamination stacks<br />

represent two-dimensional values typically<br />

ranging between 1500 and 5000, whereas the<br />

isotropic IP grades approach ~500 permeability.<br />

Some conversions may necessitate higher input<br />

current to achieve similar flux density. However,<br />

3-dimensional flux paths provide greater design<br />

and performance flexibility. In addition, use of<br />

high-energy permanent magnet materials can<br />

compensate for the lower permeability of the<br />

soft magnetic composite grades.<br />

Induction Influences the ultimate torque<br />

capability of rotating machines. Lower values<br />

can be offset by increasing the backing section<br />

(material mass), while maintaining optimal<br />

component packaging associated with<br />

optimized end-winding and slot fill.<br />

Strength In some instances, components must<br />

withstand rotational forces, stresses associated<br />

with press fitting or compression joining, and<br />

have sufficient strength to accommodate the<br />

copper winding process during assembly.<br />

Appropriate polymer types and process<br />

conditions permit adequate strength to support<br />

application requirements.<br />

AC Frequency Preferred applications involve<br />

operating conditions of 200 Hz electrical<br />

frequency. This utilizes the benefits associated<br />

with the inherently low eddy current losses of<br />

I.P. materials.<br />

Core-Loss The two primary components of<br />

core-loss include eddy current and hysteresis<br />

losses. Greater core-loss values generally<br />

increase operating temperatures, which leads to<br />

additional losses. Lower loss values translate<br />

into greater electrical efficiencies. Losses can be<br />

minimized with proper particle coating, binder<br />

combinations and stress relief.<br />

Processing Conditions Various options exist<br />

depending upon the binder and/or lubricant<br />

combinations. Warm compaction, with or<br />

without powder heating, or conventional<br />

compaction can be used for a variety of<br />

applications.<br />

Base Iron Chemical composition and particle<br />

size, along with component density, can be<br />

manipulated to enhance specific magnetic<br />

performance characteristics.<br />

Curing Temperature A secondary thermal<br />

treatment enhances the binder strength and<br />

helps minimize internal stress promoting<br />

recovery of the iron powder crystal structure.<br />

Temperature optimization is required to limit<br />

internal stresses without destroying the binder<br />

characteristics.


MAGNETIC TERMINOLOGY<br />

Induction (B) is the magnetic flux per unit area,<br />

measured in Gauss. Sometimes referred to as<br />

flux density. This characteristic has a direct<br />

relationship with component density.<br />

Permeability (µ) essentially indicates the ease<br />

with which a material can be magnetized or its<br />

magnetic sensitivity – represents a ratio of flux<br />

density to magnetizing force.<br />

Coercive Field Strength (Hc ) is the<br />

demagnetizing force necessary to restore the<br />

magnetic induction to zero.<br />

Eddy Current Loss is the primary component<br />

of high frequency loss. Generally associated<br />

with electrical currents that create an opposing<br />

force to the magnetic flux when exposed to AC<br />

fields. Higher resistivity values are beneficial in<br />

minimizing eddy current losses.<br />

Hysteresis Loss represents the primary loss<br />

factor at lower frequency, and is primarily<br />

attributed to magnetic friction in the core. Wider<br />

and taller B-H loop areas generally represent<br />

greater hysteresis loss for a given material.<br />

Intrinsic Saturation is the point at which all the<br />

domains in the magnetic material become<br />

oriented in the same direction as the applied<br />

field energy.<br />

Magnetizing Force (H) is the applied energy to<br />

induce magnetic flux, measured in Oersteds.<br />

Hysteresis Curve is the measurement technique<br />

representing the closed circuit of a magnetic<br />

material subjected to positive and negative<br />

magnetizing forces – graphically represents<br />

the material’s magnetic characterization,<br />

i.e., saturation, residual induction and coercive<br />

field strength.<br />

Soft Magnetic components have the ability to<br />

both store or strengthen magnetic energy and<br />

allow for easy conversion back into electrical<br />

energy - often utilized to strengthen the<br />

magnetic flux of an electric device as a core<br />

product.<br />

Hard Magnets represent greater coercivity<br />

levels and are difficult to demagnetize, typically<br />

referred to as permanent magnets and<br />

represent a broad B-H curve band-width<br />

(>M.M.F.).<br />

Air Gap represents a low permeability gap<br />

(air space) in the flux path of a magnetic circuit,<br />

generally undesirable for energy transfer –<br />

however, can be beneficial to increase the<br />

ability to store energy in a core.<br />

Reluctance essentially represents magnetic<br />

circuit “resistance,” which is inversely<br />

proportional to permeability and directly<br />

proportional to magnetic circuit length.<br />

Ferrites are combinations of iron oxides with<br />

Mn, Zn, Ni used when high permeability and<br />

low eddy current losses are desirable, generally<br />

exhibit low saturation induction – generally used<br />

for high frequency 10 KHz to 1 GHz applications.<br />

Laminations are low carbon steel or silicon-iron<br />

grades made in thin strips with insulation<br />

coating positioned between layered stacks,<br />

extensively used in low 60 Hz electric motor<br />

applications because of low cost and design<br />

familiarity.<br />

Iron <strong>Powder</strong> Cores share some characteristics<br />

with <strong>Insulated</strong> <strong>Powder</strong> grades. They are<br />

primarily used for energy storage, transformers<br />

and inductors in various consumer products.<br />

Q Factor is a means of determining the<br />

effectiveness of an iron core – represents a ratio<br />

of the increase in effective inductance to the<br />

increase in the equivalent resistance of the<br />

magnetic circuit: Q = I / R (I= increase in test<br />

coil inductance, R = core-losses).<br />

Hysteresis curve<br />

representative<br />

of a soft magnet<br />

material


Hoeganaes Corporation<br />

1001 Taylors Lane<br />

Cinnaminson, NJ 08077-2017<br />

Phone: 856.829.2220 • Fax: 856.786.2574<br />

www.hoeganaes.com<br />

© 2010 Hoeganaes Corp. All Rights Reserved. Form HEG-750-P

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