This series has 40 standard constructions with a copper cross-section from 0.5 to 20 mm². A 0.25 mm strand is optimal up to 15 kHz — at these frequencies the litz wire delivers the highest winding Q factor by minimizing the skin and proximity effects. For higher-frequency tasks you move to a 0.2 mm strand; for lower frequencies, —. All constructions are manufactured by DIADA LLC (Diada-Electro) to TU 27.32.11-019-59596873-2025 and are available in 50+ insulation grades — from PTFE and polyimide to rectangular forming.
| Designation | Strands | Cross-section, mm² | Ø, mm | Mass, kg/km | R, Ω/km |
|---|---|---|---|---|---|
| 10×0.25 | 10 | 0.5 | 1.218 | 4.664 | 35.49 |
| 21×0.25 | 21 | 1 | 1.766 | 9.794 | 16.9 |
| 31×0.25 | 31 | 1.5 | 2.145 | 14.458 | 11.45 |
| 40×0.25 | 40 | 2 | 2.437 | 18.656 | 8.87 |
| 51×0.25 | 51 | 2.5 | 2.751 | 23.786 | 6.96 |
| 62×0.25 | 62 | 3 | 3.034 | 28.917 | 5.72 |
| 72×0.25 | 72 | 3.5 | 3.269 | 33.581 | 4.93 |
| 82×0.25 | 82 | 4 | 3.489 | 38.245 | 4.33 |
| 92×0.25 | 92 | 4.5 | 3.695 | 42.909 | 3.86 |
| 102×0.25 | 102 | 5 | 3.891 | 47.573 | 3.48 |
| 112×0.25 | 112 | 5.5 | 4.077 | 52.237 | 3.17 |
| 122×0.25 | 122 | 6 | 4.256 | 56.901 | 2.91 |
| 133×0.25 | 133 | 6.5 | 4.443 | 62.031 | 2.67 |
| 143×0.25 | 143 | 7 | 4.607 | 66.695 | 2.48 |
| 153×0.25 | 153 | 7.5 | 4.766 | 71.359 | 2.32 |
| 163×0.25 | 163 | 8 | 4.919 | 76.023 | 2.18 |
| 174×0.25 | 174 | 8.5 | 5.082 | 81.154 | 2.04 |
| 184×0.25 | 184 | 9 | 5.226 | 85.818 | 1.93 |
| 194×0.25 | 194 | 9.5 | 5.366 | 90.482 | 1.83 |
| 204×0.25 | 204 | 10 | 5.503 | 95.146 | 1.74 |
| 213×0.25 | 213 | 10.5 | 5.623 | 99.343 | 1.67 |
| 225×0.25 | 225 | 11 | 5.779 | 104.94 | 1.58 |
| 235×0.25 | 235 | 11.5 | 5.906 | 109.604 | 1.51 |
| 245×0.25 | 245 | 12 | 6.031 | 114.268 | 1.45 |
| 255×0.25 | 255 | 12.5 | 6.152 | 118.932 | 1.39 |
| 265×0.25 | 265 | 13 | 6.272 | 123.596 | 1.34 |
| 275×0.25 | 275 | 13.5 | 6.389 | 128.26 | 1.29 |
| 285×0.25 | 285 | 14 | 6.504 | 132.924 | 1.25 |
| 296×0.25 | 296 | 14.5 | 6.629 | 138.054 | 1.2 |
| 306×0.25 | 306 | 15 | 6.74 | 142.718 | 1.16 |
| 316×0.25 | 316 | 15.5 | 6.849 | 147.382 | 1.12 |
| 325×0.25 | 325 | 16 | 6.946 | 151.58 | 1.09 |
| 336×0.25 | 336 | 16.5 | 7.062 | 156.71 | 1.06 |
| 345×0.25 | 345 | 17 | 7.156 | 160.908 | 1.03 |
| 357×0.25 | 357 | 17.5 | 7.28 | 166.505 | 0.99 |
| 366×0.25 | 366 | 18 | 7.371 | 170.702 | 0.97 |
| 378×0.25 | 378 | 18.55 | 7.491 | 176.299 | 0.94 |
| 388×0.25 | 388 | 19 | 7.589 | 180.963 | 0.91 |
| 399×0.25 | 399 | 19.58 | 7.696 | 186.094 | 0.89 |
| 408×0.25 | 408 | 20 | 7.782 | 190 | 0.87 |
Three parameters drive the choice: frequency (sets the strand diameter), current (sets the copper cross-section), and temperature and environment (set the insulation grade). We work backwards: frequency first — it unambiguously narrows the series.
The copper skin depth falls as frequency rises. Once it becomes comparable to the strand radius, a thicker strand stops helping — you need a thinner one.
| Frequency | Strand diameter |
|---|---|
| up to 15 kHz | 0.25 mm |
| up to 25 kHz | 0.2 mm |
| up to 50 kHz | 0.15 mm |
| up to 100 kHz | 0.1 mm |
| up to 200 kHz | 0.071 mm |
| above 200 kHz | 0.05 mm (made to order) |
This series — 0.25 mm, up to 15 kHz.
For transformer and inductor windings, a typical current density is 3–5 A/mm² (depending on the cooling regime and the allowable temperature rise).
| Operating current | Cross-section |
|---|---|
| 2–3 A | 0.5 mm² |
| 4–6 A | 1 mm² |
| 7–10 A | 2 mm² |
| 15–20 A | 4 mm² |
| 30–40 A | 8 mm² |
| 60–80 A | 16 mm² |
For an accurate calculation, account for the waveform (sine / PWM / pulse) — it sets the RMS value and the losses.
Once the cross-section is set, you choose the grade — it determines the operating temperature, chemical resistance, breakdown voltage and cross-section shape.
Not sure — use the winding calculator: it picks the nearest standard construction for your turns count, inductance and current. Or read the article on skin effect and proximity effect — with formulas and examples.
The frequency-range boundaries are calculated by the Sullivan criterion d ≤ δ/2 (copper skin depth δ = 2.09/√f[kHz] mm). Source: Sullivan C.R., Zhang R.Y. "Simplified Design Method for Litz Wire" — IEEE APEC 2014.
Popular versions — the full catalog is on the "Products" page (50+ grades).
Our engineers will help you select the optimal construction and insulation grade for your task