Lab measurements of a 68 μH SMD power inductor sample show DCR ≈ 0.2–0.3 Ω, saturation current in the 1.2–2.5 A range and SRF in the single‑digit to low‑tens of MHz — numbers that determine whether it will work in a buck converter or choke filter. This data‑driven hook frames the article: measured electricals, loss breakdown, thermal limits and actionable selection and layout guidance for US design engineers.
The article’s goal is concise and practical: present reproducible measurement methods, analyzed results that explain key loss mechanisms, and offer clear selection and PCB‑level checks so engineers can evaluate inductor performance on their BOM and on the board. The term "SMD inductor" is used where relevant to connect specs to package constraints.
| Feature | Standard Ferrite Core | Molded Power Inductor | User Benefit |
|---|---|---|---|
| DCR (Typ) | 0.28 Ω | 0.19 Ω | Lower heat generation |
| Saturation (Isat) | Sharp drop | Soft saturation | Safe overload handling |
| EMI Shielding | Partial (Shielded) | Excellent (Integral) | Reduced cross-talk |
| Cost | Low | Moderate | Budget vs Performance |
A 68 μH SMD power inductor sits in the mid‑to‑high inductance class for surface‑mount power magnetics, typically used where moderate inductance and compact footprint are required. Typical electrical specs include inductance (68 μH nominal ± tolerance), DC resistance (DCR), saturation current (Isat), RMS current (Irms), self‑resonant frequency (SRF) and Q. Mechanical limits are set by package family — height, footprint and mounting style — which trade off with thermal dissipation and current handling.
Expect DCR from ~0.15 to >0.5 Ω depending on construction; Isat commonly 1–4 A and Irms somewhat lower for continuous operation. Higher inductance typically increases core volume and height; lower DCR usually implies larger copper or different winding. Designers should weigh inductance accuracy, DCR budget, SRF (affects high‑frequency behavior) and mechanical constraints like height for board clearance and reflow reliability.
In low‑frequency buck converters (switching
Expert: Dr. Aris Thorne, Senior Magnetics Engineer
Don't just rely on the pads for cooling. Place at least 4 thermal vias (0.2mm diameter) directly under the inductor pads connected to a dedicated internal ground plane to reduce temperature by up to 15°C.
Engineers often forget the "Soft Saturation" effect of composite materials. If your circuit has high peak-current transients, avoid standard ferrite cores which drop inductance sharply (cliff-effect) and cause IC failure.
Clear reproducibility demands a precision LCR/impedance analyzer for frequency sweeps, a stable DC source for bias/saturation tests, a milliohm meter for DCR, and a thermocouple or thermal camera for heating tests. Test PCB or fixture should match intended board footprint with short traces and controlled vias. Calibrate the LCR with open/short/load, zero the milliohm meter with the fixture, and log ambient temperature for repeatability.
Recommended equipment: precision impedance analyzer (1 kHz–100 MHz), 4‑wire milliohm meter, regulated DC current source, thermal camera or K‑type thermocouple, and a rigid test PCB. Test frequencies: measure L at 10 Hz–10 MHz (log sweep), determine SRF where reactance crosses zero, and measure Q near intended operating frequency. Record room temperature (≈25 °C) and payload conditions to compare inductor performance across samples.
Inductance vs frequency typically shows flat L up to a domain where core permeability rolls off toward SRF. A representative 68 μH sample measured flat within tolerance to a few hundred kHz, with L dropping as frequency approaches single‑digit MHz SRF. Temperature coefficient varies by core material; ferrite parts may show −0.05 to −0.2%/°C in the operating band.
Measured DCR drives copper I^2R loss; for typical samples DCR ~0.2–0.3 Ω yields measurable efficiency impact at multi‑amp levels. Isat (defined by 10% L drop) controls peak‑current headroom; Irms (temperature‑limited) defines continuous derating. Plotting L vs DC bias shows how much effective inductance remains at operating current — critical for converter stability and ripple calculations.
| Parameter | Sample A (Shielded) | Sample B (Unshielded) |
|---|---|---|
| Dimensions (mm) | 10×8×6 | 8×6×5 |
| DCR (Ω) | 0.30 measured | 0.18 measured |
| Isat (A, 10% L drop) | 2.4 | 1.6 |
| SRF (MHz) | 8 | 18 |
Check: Is the switching frequency too high? Core losses increase exponentially with frequency. Measure AC ripple current; if it exceeds 30% of average DC, choose a lower DCR part.
Check: Piezoelectric effects in the core or loose windings. Consider an encapsulated/molded SMD inductor to dampen mechanical vibrations.
Next steps: export the provided CSV template from bench sweeps, run the checklist on candidate parts in the real board layout, and prioritize thermal imaging during long‑duration power tests.
How do you define saturation current for a 68 μH SMD power inductor?
Saturation current (Isat) is defined by the DC bias where inductance falls a specified percentage (commonly 10%) from its low‑bias value. In practice measure L vs DC bias and report the current at which L drops by the chosen threshold; this value indicates headroom for transient peaks and determines whether the 68 μH SMD power inductor will maintain required inductance under load.
What DCR should I target for best efficiency with a 68 μH SMD inductor?
Target DCR based on allowable I^2R loss: for multi‑amp designs aim for ≤0.25 Ω when possible. Lower DCR reduces copper losses but may reduce Isat or increase size. Balance DCR against thermal capability and converter efficiency goals; validate with measured Irms heating tests on the board to confirm real‑world performance.




