Contact Transmart
You have spent 3 months designing a compact, elegant power supply for a very advanced electronic device. You start it up, run it under stress and it appears OK for approximately 10 minutes. After that, the temperatures rise, the efficiency falls dramatically and the entire system shuts down because of overheating.
What went wrong? You used a traditional magnetic core which could not withstand high frequencies.
As you scale up the operating frequency to make power electronics smaller, lighter and more efficient, standard magnetic cores become miniscule heaters. The selection of the appropriate soft magnetic materials is the most critical in today's high frequency design.
This article will explain the working principles of high frequency magnetic materials, the types of materials available and how to select the right core for your project.
Let's keep things simple with the basic definition, before we head into high frequencies. A soft magnetic material is a material with a large magnetic susceptibility; it can be magnetized easily through a magnetic field acting on it, but it quickly loses magnetic characteristics when this field is removed.
These materials do not dissipate much energy as heat because they can change their magnetic direction millions of times per second without any resistance. That reset is quick and that's why they are vital for today's alternating current (AC) electronics. You'll see them working silently in the cores of power transformers, electric motors, and high-speed energy storage inductors.
Standard silicon steel works fine at standard low frequencies, such as 50Hz or 60Hz power coming directly from a wall socket. It maintains a strong magnetic field, has a slow switching rate and remains fairly cool.
However, at higher frequency (hundreds of kilohertz (kHz) or megahertz (MHz)), the core undergoes physical modifications:
To achieve a cool and efficient electronic system, you must select soft magnetic materials which are specially made to minimize such losses at high frequencies.
Each material has its own set of benefits for different frequency bands, dimensions, and power levels. Let's break down the most common material choices.
|
Material Type |
Frequency Range |
Saturation Flux Density (Bs) |
Core Loss at High Frequency |
Best Used For |
|
Ferrites (MnZn & NiZn) |
100 kHz - 100+ MHz |
Low (0.3 - 0.5 T) |
Very Low |
High-frequency signal transformers, RF circuits, small inductors |
|
Amorphous Alloys |
20 kHz - 100 kHz |
Medium-High (1.2 - 1.5 T) |
Low |
Medium-frequency distribution transformers, choke coils |
|
Nanocrystalline Alloys |
10 kHz - 200+ kHz |
High (1.2 T) |
Very Low |
High-power transformers, common mode chokes, EV chargers |
|
Powdered Metal Cores |
50 kHz - 1 MHz |
High (1.0 - 1.6 T) |
Moderate |
DC output chokes, power factor correction (PFC) inductors |
Ferrites are ceramic oxides manufactured by sintering iron oxide with other metals such as manganese, zinc or nickel.
Nanocrystalline ribbons are prepared by rapidly cooling molten Fe-based alloys into thin ribbons then annealed to achieve a uniform microscopic grain size of approximately 10 nm.
Amorphous metals are formed by rapid cooling of the liquid alloy, in which no crystal structure has sufficient time to grow. This results in a non-crystalline flexible metallic ribbon.
Powdered cores are created by coating microscopic grains of a metal alloy such as iron-silicon-aluminum or nickel-iron with a forming binder and pressing it into place under a high pressure.
To select a core in your new high frequency project, this quick checklist will help you:
The switching frequency directly affects which material families are usable. The core losses increase non-linearly as frequency is raised, making it important to match the material to your desired band.
For application where high peak currents or space restrictions are involved, high saturation flux density ($B_s$) core material is required. The higher the $B_s$ value, the more magnetic energy the core can store without saturation, which means that smaller components can be designed without the concern of circuit failure.
Always verify the core loss ($P_c$) curves published by the manufacturer under your working temperature and switching frequency. Reduced core loss results in less heat generation and increased operating efficiency. More detailed core loss testing methods can be found at IEEE Xplore.
The core loss generates heat, which, accordingly, alters the magnetic permeability. Ensure that the core you choose has a uniform magnetic characteristic in your operating temperature range (typically -40° C to +125° C).
Nanocrystalline and high-grade ferrite alloys exhibit better temperature-versus-loss properties compared to iron powder forms at lower cost.
The selection of the right soft magnetic material depends essentially on three fundamental engineering parameters: operating frequency, power density and thermal limits.
With the trend of faster switching speeds to reduce size and weight, the use of dated core technologies will result in excessive heat and energy loss. Knowing the particular strengths of ferrites, nanocrystalline alloys, amorphous metals, and powdered cores allows you to choose a material to keep your system cool, compact, and efficient.
At Transmart, from lightweight nanocrystalline cores offering optimal performance in electric vehicle power applications, to low-loss ferrites ideal for high-frequency signal circuits, choosing the right core material to meet your specific frequency profile guarantees your design will function reliably over the long haul.