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High-Current DC-DC Converters: Which Inductor Trade-Offs Matter?

A flat-wire inductor may lower winding resistance through better conductor packing, but converter heat also comes from core, switching, PCB, and cooling losses. Choose against the real current waveform and operating conditions.

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A high-current DC-DC converter can run hot even when its switching devices are efficient because heat comes from losses throughout the power path. The inductor can remain a significant source: its winding dissipates heat through resistance, while its magnetic core loses energy as flux changes. Flat-wire windings can make room for more conductor and, in a suitable design, reduce winding resistance—but they cannot by themselves eliminate core loss, switching loss, or cooling and layout limits.

Why does a high-current converter still run hot?

Efficiency improvements in MOSFETs and control circuitry reduce some losses, but do not remove the energy dissipated elsewhere. Conduction and switching losses in the power stage, inductor winding and core losses, and resistance in the PCB and connections all contribute. Heat must also travel from those components into the board and surroundings; restricted airflow, a small copper area, or a hot enclosure can raise component temperatures even when losses have not changed.

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TDK identifies winding copper loss and core-material loss as two main causes of inductor temperature rise in its power-inductor application guidance. So a cooler switching stage does not necessarily mean a cool converter: the inductor and thermal path still matter.

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Where inductor heat comes from

Winding loss: current through resistance

The first-order estimate for DC winding loss is P = I² × DCR. In a buck converter, the inductor’s average current is closely related to output current, with switching ripple superimposed. Because current is squared, resistance reductions can have a meaningful effect at high current. For a more accurate estimate with ripple, use the current waveform rather than treating it as a constant DC value; Analog Devices’ efficiency primer explains this first-order approach and its limits.

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The DCR printed in a datasheet is not the whole winding-loss story. It is measured under stated conditions, and copper resistance rises as the winding heats. At switching frequencies, current distribution also becomes nonuniform: skin effect and proximity effects can increase AC winding resistance beyond the DC value. Actual winding heating therefore depends on the conductor geometry, frequency, ripple waveform, and operating temperature.

Core loss: changing magnetic flux

The core dissipates energy as magnetic flux changes. Hysteresis and eddy currents are important components, and the resulting loss depends on core material and operating conditions, including frequency and flux swing. At moderate to heavy load, winding copper loss often becomes the larger inductor contribution; at light load in constant-frequency operation, core loss may dominate. A converter can therefore run warm for different reasons at different load points.

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What flat-wire windings can improve

Round wire leaves gaps in a winding window. A flat conductor can pack that space more efficiently, potentially allowing greater conductor cross-section in a similar volume or a more compact winding. If the resulting design has lower DCR, its DC winding loss can fall. Some optimized helical geometries can also have lower AC winding resistance than a solid round-wire implementation, but that result depends on the specific winding design; flat wire alone does not guarantee it.

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The Bourns ER26A is one example of a product family described as using a helical flat-wire winding alongside magnetic shielding and a high-temperature ferrite core. Those are design features, not evidence of a particular temperature reduction or efficiency gain versus a round-wire part. The product discussion is in the published ER26A article.

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What flat wire does not fix

  • Core loss: A winding change does not remove hysteresis or eddy-current loss. Core material, flux swing, frequency, and magnetic design remain relevant.
  • Switching and conduction losses elsewhere: Changing the inductor cannot compensate for losses in the semiconductors, controller, connections, or other parts of the power path.
  • Thermal bottlenecks: A lower-loss component can still run hot if its PCB copper, airflow, mounting, or path for heat removal is inadequate.
  • EMI and stray fields: Magnetic shielding may reduce stray-field coupling, but overall EMI performance also depends on layout, grounding, switching loops, and nearby components.
  • Frequency-dependent winding loss: Flat wire does not automatically eliminate skin or proximity effects; AC resistance and field distribution still depend on the design and operating point.
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How to choose an inductor for the real operating point

Compare candidates under the same converter conditions—not just by shape, nominal current, or room-temperature DCR. Use the expected current waveform, switching frequency, temperature, board, and cooling conditions.

  1. Set inductance and ripple targets. Check that the inductance suits the topology and switching conditions, and that the resulting ripple current is acceptable.
  2. Check peak current against saturation. Compare the inductor’s peak current with the datasheet’s saturation behavior and definition. Saturation current is not interchangeable with a temperature-rise current rating.
  3. Check RMS current against heating. Use RMS current and account for ambient temperature, PCB copper, and cooling when evaluating the temperature-rise rating. TDK notes that a rated current is generally the lower of saturation-related and temperature-rise current, but the two underlying limits describe different failure mechanisms.
  4. Estimate winding loss at temperature. Use DCR at its stated test temperature and account for its increase as the winding warms. Apply the actual current waveform where ripple is material.
  5. Evaluate AC and core loss. At the actual switching frequency and ripple waveform, look for supplier loss curves or data. If the datasheet does not provide enough information, ask the manufacturer rather than assuming DC resistance predicts total inductor loss.
  6. Check fit and system implications. Compare footprint, height, core behavior, shielding and stray-field effects, cost, and availability against the design constraints. Verify the complete layout and cooling path as well as the component.

Coilcraft’s selection guidance also distinguishes peak-current saturation checks from RMS-current heating checks and notes that DCR changes with temperature.

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How to interpret published flat-wire family ranges

Published family-level ranges can help identify candidates, but they are not a promise that one part has every listed attribute at once. Eaton lists the HFW high-current flat-wire family for DC-DC converter applications with the following ranges. Confirm the exact variant’s datasheet, test conditions, and availability before using a value in a design.

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Eaton HFW family attribute Published range
Current applications 5–100 A
Inductance 2–33 μH
SMT footprints 22 mm and 28 mm
Height 10–18 mm

These are family-level ranges published on Eaton’s HFW product page, not simultaneous ratings for a single inductor. Selection still requires checking the specific part’s current ratings and operating conditions.

Product prices and availability are accurate as of the date/time indicated and are subject to change. Any price and availability information displayed on Amazon at the time of purchase will apply.

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