| Operating Frequency |
50–60 Hz for power transformers 20–500 kHz for high-frequency transformers |
Core loss generally increases with frequency. In the low-loss region, the frequency exponent commonly ranges from about 1.2 to 2.5, depending on material and waveform. |
A core designed for 50/60 Hz is normally unsuitable for operation at tens or hundreds of kilohertz. High-frequency materials require lower eddy-current losses and controlled manufacturing tolerances. |
Compare loss data at the actual operating frequency, switching waveform, duty cycle, and temperature. Do not compare a 100 kHz value with a 1 kHz value without normalization. |
| Peak Flux Density, Bpk |
Approximately 20–80 mT for many ferrite designs at high frequency Approximately 0.8–1.6 T for many 50/60 Hz electrical-steel designs |
Core loss commonly rises approximately with B1.5 to B2.7, depending on the material, frequency, and waveform. |
A small increase in flux density can create a disproportionate increase in loss. Operating too close to saturation also increases magnetizing current and distortion. |
Specify peak, peak-to-peak, or RMS flux density clearly. For asymmetric volt-seconds, check DC bias and flux walking rather than relying only on nominal turns ratio. |
| Operating Temperature |
25°C reference testing; approximately 80–120°C in many enclosed power assemblies |
Temperature effects vary by material. Ferrite loss may decrease over part of its temperature range, while resistivity, permeability, and saturation flux density also change. |
The minimum-loss temperature is not always the maximum-performance temperature. Thermal design must include both core loss and copper loss because each increases the other’s operating temperature. |
Request loss curves at the expected hot-spot temperature, not only at 25°C. Confirm the allowable temperature rise of the core, winding insulation, adhesive, and bobbin system. |
| Excitation Waveform |
Sine wave, square wave, trapezoidal wave, PWM, or resonant waveform |
At the same frequency and flux density, non-sinusoidal waveforms can produce higher loss because of harmonics, rapid transitions, and minor-loop operation. |
A datasheet value measured with a sine wave may not represent the loss in a hard-switched converter. The applied volt-second waveform should be used for design verification. |
Provide switching frequency, rise and fall time, duty cycle, dead time, DC bias, and harmonic content when requesting comparative core-loss data. |
| Material Family |
MnZn ferrite: typically high-frequency power applications Nanocrystalline or amorphous alloy: medium-to-high-frequency and high-permeability applications Electrical steel: low-frequency power applications Powdered magnetic material: distributed-gap and energy-storage applications |
Loss varies widely within each family because composition, lamination thickness, particle insulation, annealing, gap structure, and processing all affect performance. |
Material selection must balance core loss, saturation flux density, permeability, mechanical strength, thermal stability, size, and cost. |
Request the material grade, effective permeability, saturation data, density, test method, and complete loss curve. A material family name alone is not sufficient for procurement. |
| Core Geometry and Size |
E, U, C, toroidal, planar, and cut-core structures; effective volumes from small sub-cubic-centimeter parts to large power cores |
Geometry does not change the intrinsic material loss directly, but it changes flux distribution, thermal resistance, winding length, leakage fields, and local hot spots. |
An identical material can show different measured temperature rise or total loss when used in different shapes or with different winding windows. |
Compare both specific loss in W/kg or kW/m³ and total core loss in watts. Check effective magnetic length, effective cross-sectional area, volume, and mass. |
| Air Gap and DC Bias |
Ungapped cores for transformer action; intentional gaps commonly used in inductors and energy-storage components |
A gap lowers effective permeability and reduces inductance. Fringing fields near the gap can increase local winding and core losses. |
For transformer cores, unintended gaps and poor mating surfaces can increase magnetizing current. For gapped inductors, gap length and fringing must be included in the loss model. |
Specify nominal gap, tolerance, mating condition, surface finish, and DC current. Measure inductance under both zero-bias and rated-bias conditions. |
| Manufacturing Tolerance |
Commonly affected parameters include permeability, core area, path length, lamination factor, gap, and surface flatness |
Variations in dimensions and material properties can cause changes in flux density, inductance, magnetizing current, and total loss. |
A design using only typical values may pass laboratory tests but fail at production extremes. Worst-case tolerance analysis is recommended for high-volume products. |
Ask for dimensional tolerances, lot-to-lot consistency, inspection criteria, traceability, and acceptance limits for loss, inductance, and permeability. |
| Representative Loss Reference |
Specific core loss is commonly reported in W/kg or kW/m³. Typical values may range from below 1 W/kg at low-frequency power conditions to tens or hundreds of W/kg at high-frequency conditions. |
The value is meaningful only when frequency, flux density, waveform, temperature, and test method are stated together. |
For a practical estimate: Total Core Loss ≈ Specific Core Loss × Core Mass. This estimate should be corrected for waveform, DC bias, joint loss, and temperature where applicable. |
Treat any single headline loss number as a reference point rather than a universal rating. Require a complete loss map or curve for final component approval. |