400 Hz Magnetics Are Not 50 Hz Parts at Higher Frequency
Aircraft ground power units, airborne avionics, and shipboard 400 Hz systems all use transformers and inductors sized around a fundamental about eight times higher than 50 Hz. The higher frequency shrinks the core dramatically, but it simultaneously raises core loss per unit volume, changes the wire’s effective resistance through skin effect, and shifts the entire loss balance toward the core. A 400 Hz transformer built with 50 Hz design habits will be small and hot.
For buyers, the practical questions are: what core material, what winding construction, and what efficiency and temperature rise to require at 400 Hz.
Design Differences From 50 Hz
| Item | 50 Hz | 400 Hz |
|---|---|---|
| Core volume for the same VA | Reference | Roughly 25–40 % of the 50 Hz volume |
| Core material | Grain-oriented silicon steel, 0.27–0.35 mm | Thin silicon steel (0.20–0.27 mm) or high-frequency ferrite for small units |
| Flux density | 1.3–1.5 T typical | Often 1.0–1.2 T to control loss |
| Skin depth in copper | ~9.3 mm at 50 Hz | ~3.3 mm at 400 Hz; foil/strand choice matters |
| Dominant loss | Copper | Often core; balance shifts with flux choice |
| Insulation class | Class B/F common | Class H common due to smaller, hotter cores |
Aircraft and Ground Support Requirements
Airborne equipment typically follows DO-160 environmental categories (temperature, altitude, vibration, humidity) in addition to electrical requirements, while ground power units follow the local standard for 400 Hz supply, often with tight voltage and frequency tolerances. Both push toward higher insulation classes because the core is small and the surface-to-volume ratio is high, so heat is harder to dissipate.
Weight is the binding constraint in airborne units. Engineers routinely trade 1–2 % efficiency for several hundred grams, which pushes the design toward thinner laminations and higher flux at the cost of a hotter core — a trade that must be verified with measured loss, not catalog data.
Winding Construction at 400 Hz
At 400 Hz the skin depth in copper is about 3.3 mm, so round wire up to roughly 1.5 mm diameter behaves as DC; above that, or with foil, AC resistance rises unless the conductor is thin relative to skin depth. Practical rules: keep round wire below about 1.2 mm and parallel strands for higher currents; if foil is used for a high-current secondary, cap foil thickness near 0.5 mm and interleave to control proximity effect.
What to Specify
- Fundamental frequency, waveform (some 400 Hz supplies have significant harmonic content), and voltage tolerance.
- Efficiency target and the temperature rise allowed at the specified ambient.
- Core material grade and lamination thickness, with measured no-load and load loss.
- Insulation class and the required dielectric test level.
- Weight limit, if the application is airborne.
- Environmental category (DO-160 or equivalent) for temperature, altitude and vibration.
Related reading
- Laminated Core Step-Lap Stacking
- Core Loss vs Copper Loss Optimization
- Litz Wire Design
- Thermal Design of Transformers and Inductors
We build 400 Hz transformers for ground power and airborne programs with measured loss at the rated flux, thin-lamination cores, and Class H insulation where weight forces a small core. Send your VA rating, frequency tolerance, weight limit, and environmental category to sales@sirui-tech.com.
