LITZ WIRE ENGINEERING GUIDE

Choosing strand count by frequency
One rule, four steps, two worked examples

Short answer: pick a strand diameter at or below about one skin depth of your operating frequency, size the total copper cross-section from your current (3–6 A/mm² is typical at high frequency), divide one by the other to get the strand count, then verify the bunched outer diameter fits your winding space. The skin-depth table and two fully worked examples below do exactly this.

STEP 1 · FREQUENCY → STRAND DIAMETER

The skin-depth rule

In copper, skin depth in millimetres ≈ 66 / √f, with f in hertz. Keep the strand diameter at or below roughly one skin depth (0.7–1.5 δ works in practice)

Operating frequencySkin depth δ (copper)Typical strand diameter
20 kHz0.467 mm0.30–0.50 mm
50 kHz0.296 mm0.20–0.30 mm
100 kHz0.209 mm0.15–0.20 mm
200 kHz0.148 mm0.10–0.15 mm
400–500 kHz0.100–0.105 mm0.05–0.10 mm
1 MHz0.066 mm0.05 mm and finer
Why it matters Above roughly 10–20 kHz, AC current crowds toward the conductor surface. A strand much thicker than the skin depth carries current only in a thin shell, so most of its copper does nothing. Splitting the same total copper into many fine strands restores usable cross-section — that is the entire point of litz wire.
STEPS 2–4

The four-step sizing method

1 · Frequency → strand dia.

Take the strand diameter from the skin-depth table above, scaled to your exact frequency.

2 · Current → copper section

Total copper area = rated current ÷ current density. 3–6 A/mm² is typical at high frequency; tighten it for sealed or high ambient temperature windings.

3 · Section → strand count

Strand count = total copper area ÷ area of one strand. One 0.2 mm strand is 0.0314 mm², one 0.1 mm strand is 0.00785 mm². Round up to a standard construction.

4 · Check the geometry

Bunched OD ≈ 1.25 × strand dia. × √strand count. Confirm it fits the slot or bobbin and winds cleanly; if not, adjust strand diameter and repeat.

WORKED EXAMPLE A

100 kHz · 12 A — wireless power TX coil

A typical wireless charging transmitter coil specification

StepResult
Skin depth at 100 kHz0.209 mm → choose 0.20 mm strand (≈ 1 δ)
Copper section at 4 A/mm²12 A ÷ 4 = 3.0 mm²
Strand count3.0 ÷ 0.0314 = 95.5 → 100 strands × 0.20 mm
Check: actual density100 × 0.0314 = 3.14 mm² → 3.8 A/mm² ✓
Check: bunched OD1.25 × 0.20 × √100 ≈ 2.5 mm ✓
WORKED EXAMPLE B

440 kHz · 80 A — induction heating work coil

A real build we supplied, measured and verified

StepResult
Skin depth at 440 kHz0.100 mm → choose 0.10 mm strand (≈ 1 δ)
Strand count3500 strands × 0.10 mm, built as re-twisted bundles
Total copper section3500 × 0.00785 = 27.49 mm²
DC resistance0.627 mΩ/m
Continuous rating80 A in a naturally cooled winding (2.9 A/mm²); 90 A absolute max
Finished OD≈ 7.3 mm
PRACTICAL WARNINGS

Four mistakes that cost weeks

1 · Sizing by DC ampacity only

DC wire tables ignore skin and proximity effect. In a multi-layer winding above tens of kilohertz, AC resistance of a solid or coarse-stranded conductor can be several times its DC value — and your coil heats exactly where the current is.

2 · Going finer than needed

Strand diameter below the skin depth buys little, and every extra strand adds insulation and cost. Fill factor drops because a growing share of the bundle is enamel, not copper.

3 · Ignoring proximity effect

Adjacent turns and layers distort each other's field. When the winding has many layers or tight pitch, specify a multi-bundle (re-twisted) construction — bundles twist groups of strands so that each takes its share of the layers.

4 · Forgetting enamel class and serving

Thermal class 130 / 155 / 180 / 200 / 220 must match your worst-case hotspot, not your ambient. Served or yarn-covered constructions add outer diameter — include it in the slot check before ordering.

BOUNDARY CASE

When solid wire is still fine

Don't over-engineer Below roughly 10–20 kHz — or whenever the solid wire diameter is comfortably below one skin depth — a solid round wire performs essentially the same as litz. At 20 kHz (δ = 0.467 mm) a solid wire of 0.3–0.4 mm is fine. Litz wire starts paying for itself from tens of kilohertz upward, and it becomes mandatory once thermal behaviour or efficiency targets cannot be met otherwise.
FAQ

Questions engineers actually ask

Can I mix strand diameters in one conductor?

Possible but uncommon. Standard constructions keep one strand diameter throughout — bunching stays uniform and soldering predictable. If a single diameter cannot meet loss and flexibility targets, the usual fix is a multi-bundle (re-twisted) construction, not mixed strands.

How much AC resistance does litz actually save?

When strands are sized near one skin depth, the AC/DC resistance ratio stays close to 1.1–1.3 even in multi-layer windings. The same total copper as a solid wire can see several-fold higher AC resistance at the same frequency. Exact numbers depend on layer count and pitch, which is why ampacity confirmation is worth doing per design.

Is 1000+ strands practical to manufacture?

Yes, as re-twisted bundles. The 3500-strand example above is a production build with a 7.3 mm finished OD. Strand counts of 20–1000+ are routine; the practical limit is usually winding space, not manufacturability.

What should I send for a free calculation?

Operating frequency, rated RMS current, temperature-rise target, available slot or bobbin space, enamel thermal class, and any preference for serving or self-bonding. Send it on the litz wire page and the strand calculation with a quotation usually comes back within 48 hours.

SKIP THE MATH

Send frequency and current — we do the rest

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