Technical Reference

Core Materials Guide

The core is the magnetic heart of every inductor and transformer. Its material determines permeability, saturation, frequency response, and loss characteristics. This guide covers the three core materials we work with and how to choose between them.

Fundamentals

What a Core Does

A magnetic core concentrates and channels magnetic flux generated by current flowing through a wire coil. The core material amplifies the inductance of the coil by a factor equal to its relative permeability. A core with a permeability of 10,000 produces 10,000 times the inductance of an air-wound coil with the same geometry.

Material choice affects every electrical parameter: how much energy the component stores, the frequency range it operates in, how much heat it generates under AC excitation, and the current level at which the core saturates and stops functioning as designed.

Key Properties

What to Evaluate When Selecting a Core Material

μ

Permeability

The material's ability to concentrate magnetic flux. Higher permeability means more inductance per turn, reducing the number of turns needed. Ranges from 2,000 (ferrite) to over 100,000 (1J85 Permalloy).

B

Saturation Flux Density

The maximum magnetic field the core can carry before it stops responding linearly. Silicon-iron saturates at 1.6 to 2.0 Tesla. Ferrite saturates at 0.3 to 0.5 Tesla. This determines maximum operating current.

f

Core Loss

Energy dissipated as heat during AC operation. Core loss includes hysteresis loss (from the B-H loop area) and eddy current loss (from induced currents in the core). Lower loss means higher efficiency and less thermal stress.

Core Material

Ferrite Cores

Ferrite is a ceramic compound made from iron oxide (Fe2O3) mixed with manganese, zinc, or nickel oxides. The material is pressed and sintered at high temperature into a dense, brittle structure. Ferrite is the most widely used core material in electronics.

Composition: Iron oxide ceramic (MnZn or NiZn formulations)

Properties

Permeability
2,000 to 15,000
Saturation
0.3 to 0.5 T
Resistivity
Very high
Frequency Range
10 kHz to 5 MHz+
Eddy Current Loss
Very low
Temperature Stability
Moderate

Why Ferrite Works at High Frequency

Ferrite's electrical resistivity is roughly a million times higher than metallic core materials. High resistivity blocks eddy currents, which are the primary source of core loss at high frequencies. This makes ferrite the natural choice for any application operating above 10 kHz.

MnZn ferrites are optimized for frequencies from 10 kHz to about 2 MHz. NiZn ferrites extend usable frequency into the 10 MHz range and beyond, with lower permeability but higher resistivity.

Applications

  • Switching power supplies (SMPS)
  • EMI suppression filters and common mode chokes
  • Flyback and forward converter transformers
  • RF inductors and broadband transformers
  • LED driver power stages
  • Telecom power conditioning

Limitations

  • Low saturation flux density (0.3 to 0.5 T) limits current handling
  • Brittle ceramic structure, vulnerable to mechanical shock
  • Permeability drops significantly at elevated temperatures
  • Requires larger core volume for high-energy storage applications

Our Ferrite Core Specs

We work with ferrite cores from 0.878" to 1.424" OD (22 to 36 mm), including manufacturer part ZW-43610-TC. Permeability ratings across our production range from 750 to 15,000. All cores are RoHS compliant.

Core Material

Silicon-Iron Cores (Microsil)

Grain-oriented 3% silicon-iron is a metallic alloy engineered for high saturation flux density. The silicon content reduces hysteresis loss and increases electrical resistivity compared to pure iron. Grain orientation aligns the crystal structure along the rolling direction, maximizing permeability in the preferred flux path.

Composition: 3% silicon, 97% iron (grain-oriented electrical steel)

Properties

Permeability
30,000 to 50,000
Saturation
1.6 to 2.0 T
Tape Thickness
0.007" / 0.178 mm
Frequency Range
50 Hz to 10 kHz
Eddy Current Loss
Moderate (reduced by lamination)
Temperature Stability
Excellent

Why Lamination Matters

Silicon-iron is electrically conductive. In a solid chunk, alternating magnetic fields would induce large eddy currents and waste energy as heat. Tape winding solves this by building the core from thin strips of material separated by insulation.

Our silicon-iron cores use 0.007" (9 mil) tape thickness. Thinner laminations mean smaller eddy current loops and lower loss. The trade-off is that thinner tape is more expensive to process and results in a lower stacking factor (less magnetic material per unit volume).

Applications

  • Current sensing at line frequency (50/60 Hz)
  • Power transformers for mains-frequency conversion
  • Filter chokes in AC/DC power supplies
  • Energy metering current transformers
  • Motor drive output filtering
  • Industrial power monitoring

Limitations

  • High eddy current loss above 10 kHz makes it impractical for high-frequency switching
  • Heavier than ferrite for equivalent volume
  • Requires tape winding or stamped laminations, adding manufacturing cost
  • Grain orientation is directional, limiting core geometry to toroids and C-cores

Our Silicon-Iron Core Specs

We produce tape-wound silicon-iron toroidal cores from 0.8" to 2.25" OD (20 to 57 mm). Tape thickness: 0.007" (9 mil). Core heights from 0.256" to 0.500" (6.5 to 12.7 mm). Available with epoxy coating (0.015" thick) or powder coat finish. Also known as Microsil. All cores RoHS compliant.

Core Material

Permalloy (1J85) Cores

1J85 is a nickel-iron alloy containing approximately 80% nickel and 20% iron, commonly known as Permalloy or Mu-metal. It delivers extremely high initial permeability, making it the go-to material for applications requiring maximum sensitivity and signal accuracy.

Composition: ~80% Nickel, ~20% Iron (Ni-Fe alloy)

Properties

Permeability
100,000+
Saturation
0.7 to 0.8 T
Resistivity
Moderate
Frequency Range
DC to 100 kHz
Core Loss
Very low at low frequencies
Linearity
Excellent at low flux levels

Why Permeability Over 100,000 Matters

In current sensing applications, the transformer must accurately reproduce a scaled-down version of the primary current. Any loss of magnetic coupling between primary and secondary reduces accuracy. A core with permeability above 100,000 achieves near-ideal coupling at very low current levels.

This ultra-high permeability also means fewer turns are needed to achieve a given inductance, which reduces winding resistance and the physical size of the component. For precision measurement circuits, the difference between a 15,000 permeability ferrite and a 100,000+ permeability 1J85 core is the difference between 2% accuracy and 0.1% accuracy.

Applications

  • Precision current transformers for metering and monitoring
  • Magnetic shielding enclosures
  • DC current sensors and Hall-effect hybrid sensors
  • Ground fault detection circuits
  • Fluxgate magnetometers and compass sensors
  • Low-level signal transformers

Limitations

  • Low saturation flux density (0.7 to 0.8 T) limits current capacity
  • Significantly more expensive than ferrite or silicon-iron
  • Sensitive to mechanical stress (permeability degrades if the core is strained)
  • Requires careful annealing during manufacturing to achieve rated permeability

Our 1J85 Core Specs

We source 1J85 (Permalloy) toroidal cores with epoxy coating. Currently in production for precision current sensing applications with OD ranging from 0.8" to 2.5" (20 to 63 mm). Permeability verified at 100,000+ per unit. All cores RoHS compliant.

Side-by-Side Comparison

Three Core Materials, Three Performance Profiles

Property Ferrite Silicon-Iron (Microsil) Permalloy (1J85)
Permeability 2,000 to 15,000 30,000 to 50,000 100,000+
Saturation Flux Density 0.3 to 0.5 T 1.6 to 2.0 T 0.7 to 0.8 T
Optimal Frequency Range 10 kHz to 5 MHz+ 50 Hz to 10 kHz DC to 100 kHz
Core Loss at High Frequency Very Low High Moderate
Core Loss at Low Frequency Low Low Very Low
Relative Cost Low Medium High
Best Applications SMPS, EMI Filtering, RF Power Transformers, Line-Frequency Current Sensing Precision Current Sensing, Shielding
Construction Pressed & sintered ceramic Tape wound (0.007" lamination) Tape wound, annealed

Visual Comparison

Property Comparison by Material

Permeability (Relative Scale)

Ferrite 2,000 to 15,000
Silicon-Iron 30,000 to 50,000
Permalloy (1J85) 100,000+

Saturation Flux Density

Ferrite 0.3 to 0.5 T
Silicon-Iron 1.6 to 2.0 T
Permalloy (1J85) 0.7 to 0.8 T

High-Frequency Performance

Ferrite Excellent
Silicon-Iron Poor
Permalloy (1J85) Moderate

Relative Cost

Ferrite Lowest
Silicon-Iron Medium
Permalloy (1J85) Highest

Selection Guide

Which Core Material for Your Application?

Start with your application requirements. The operating frequency and the required current capacity will narrow the decision in most cases.

Choose Ferrite. Ferrite's ceramic structure provides the high resistivity needed to suppress eddy currents at switching frequencies. MnZn ferrite covers 10 kHz to 2 MHz. NiZn ferrite extends to 10 MHz and beyond. Saturation is lower (0.3 to 0.5 T), so verify that your peak current stays within the core's flux capacity.

Choose Silicon-Iron (Microsil). With saturation flux density of 1.6 to 2.0 Tesla, silicon-iron handles the highest current loads of any core material we offer. The 3% silicon addition reduces loss at mains frequency. Grain orientation maximizes permeability along the flux path. Ideal for power transformers, line-frequency filter chokes, and energy metering CTs.

Choose Permalloy (1J85). Permeability above 100,000 provides near-ideal magnetic coupling between primary and secondary windings. This translates directly to measurement accuracy. For current transformers measuring building power, industrial equipment loads, or utility metering, 1J85 delivers the linearity and sensitivity the application demands.

This is the transition zone where both ferrite and silicon-iron can work. If high saturation matters (high current, large energy storage), lean toward silicon-iron. If low core loss matters (high efficiency, low thermal budget), lean toward ferrite. Send us your spec and we can model both options.

Choose Permalloy (1J85). High permeability materials are the most effective at diverting external magnetic fields away from sensitive components. Mu-metal (another name for this alloy family) is the standard material for magnetic shielding in medical imaging, scientific instruments, and defense electronics.

Core Finishing

Core Coatings and Why They Matter

Bare metal cores require insulation between the core surface and the wire winding. Coatings also protect the core from environmental damage during handling and service life.

Epoxy Coating

Applied at 0.015" (0.381 mm) thickness. Provides electrical insulation, mechanical protection, and moisture resistance. The coating is applied uniformly and cured at temperature to create a hard, durable shell. Standard for our silicon-iron and 1J85 cores used in current sensing applications.

0.015" Thickness

Powder Coat

Electrostatically applied dry powder, cured at high temperature. Creates a thicker, more rugged finish suitable for cores that will be handled during assembly or exposed to industrial environments. Used on larger tape-wound toroidal cores where additional mechanical protection is needed during winding operations.

High Durability

Mylar Tape Wrapping

In addition to core coatings, we wrap cores in Yellow Mylar tape (3M Type 74) when the specification calls for it. Mylar provides an additional insulation layer between the core surface and the wire winding, and is standard practice for toroidal inductors in production applications.

Gallery

Cores in Production

Need help selecting the right core material?

Send us your specifications and operating parameters. We will recommend the core material, geometry, and coating that fits your application.

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