Recent bench testing shows that measured inductance under DC bias and actual RDC values frequently determine real-world converter behavior more than nominal datasheet numbers. In practice, a power inductor that meets a catalog L at zero-bias can still underperform once biased and heated on-board. This report explains how to measure inductance and RDC, typical deviations, and practical actions for designers and buyers.
Inductance and RDC set ripple magnitude, transient energy, peak currents, EMI, and copper losses. Ripple current ΔI relates inversely to L and switching frequency; I²R defines copper loss.
ΔI = (Vsw · D) / (L · fsw)
Pcu = I_RMS² · RDC
Datasheets report inductance and RDC under specific test conditions (e.g., 25°C, specific frequency) that may not match system use. Missing DC-bias curves or unspecified fixture details cause discrepancies between lab values and real-world performance.
* Recommendation: Always request L vs. DC-bias curves and fixture descriptions from suppliers.
Core materials respond differently to bias. Ferrite cores often show pronounced L reduction under bias, while powdered cores tend to be more linear.
Copper's temperature coefficient (~0.4%/°C) raises RDC with heat. At high frequencies, skin and proximity effects increase effective resistance beyond DC RDC.
A 50°C rise in temperature results in a ~20% increase in RDC. Designers must budget for realistic on-board resistance rather than catalog nominals.
| Bias Current (A) | Nominal L (µH) | Measured L (µH) | Deviation (%) | Measured RDC (mΩ) |
|---|---|---|---|---|
| 0.0 (Baseline) | 10.0 | 9.85 | -1.5% | 12.4 |
| 5.0 (50% Isat) | 10.0 | 8.92 | -10.8% | 12.5 |
| 10.0 (100% Isat) | 10.0 | 6.40 | -36.0% | 12.7 |
* Highlighted cells flag parts needing further review or larger design margins.




