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Magnetic core
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==== Iron ==== Powdered iron is the cheapest material. It has higher core loss than the more advanced alloys, but this can be compensated for by making the core bigger; it is advantageous where cost is more important than mass and size. Saturation flux of about 1 to 1.5 tesla. Relatively high hysteresis and eddy current loss, operation limited to lower frequencies (approx. below 100 kHz). Used in energy storage inductors, DC output chokes, differential mode chokes, triac regulator chokes, chokes for [[power factor]] correction, resonant inductors, and pulse and flyback transformers.<ref name="coilws"/> The binder used is usually epoxy or other organic resin, susceptible to thermal aging. At higher temperatures, typically above 125 °C, the binder degrades and the core magnetic properties may change. With more heat-resistant binders the cores can be used up to 200 °C.<ref name="chalmers">{{cite web|author=Johan Kindmark, Fredrik Rosén |url=http://publications.lib.chalmers.se/records/fulltext/183920/183920.pdf |title=Powder Material for Inductor Cores, Evaluation of MPP, Sendust and High flux core characteristics |publisher=Department of Energy and Environment, Division of Electric Power Engineering, Chalmers University of Technology |location=Göteborg, Sweden |date=2013 |access-date=2017-06-05}}</ref> Iron powder cores are most commonly available as toroids. Sometimes as E, EI, and rods or blocks, used primarily in high-power and high-current parts. Carbonyl iron is significantly more expensive than hydrogen-reduced iron.
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