Coil from a wire gauge
Wind this coil from this wire: how many turns fit, and what does it measure?
- L
- Inductance (µH, with the lengths in metres), µH
- a
- Mean winding radius, in metres, m
- N
- Turns
- ℓ
- Winding length, in metres, m
- c
- Winding depth, in metres, m
LaTeX
L = \frac{31.5 \cdot a^{2} \cdot N^{2}}{6 \cdot a + 9 \cdot ℓ + 10 \cdot c}
Method
- Look up the gauge: its insulated diameter (heavy-build enamel), its bare copper diameter, and copper's resistance per metre at that diameter.
- Turns per layer is the winding length times the packing factor, divided by the insulated diameter, rounded down — a fraction of a turn does not fit. Multiply by the layers for N.
- The winding depth is the layers times the insulated diameter, and the mean radius is the former's radius plus half that depth.
- Wire length is N turns of circumference at the mean radius; resistance is that length times the gauge's ohms per metre.
- Wheeler's multilayer formula, 0.8 a²N² ÷ (6a + 9ℓ + 10c) in microhenries with a, ℓ and c in inches, is used here with the lengths in metres, which turns 0.8 into 0.8 ÷ 0.0254 = 31.5.
- The continuous current is the bare copper's cross-section times 4 A/mm², the usual figure for a coil in air that is allowed to run warm but not hot.
Assumptions
- Orthocyclic-ish winding: each layer is the same number of turns laid side by side, and the layers stack one insulated diameter apart. A scramble wind packs worse and stands off further; the packing factor absorbs the first, not the second.
- Wheeler's 1928 multilayer formula is good to about 1 % while the winding depth and length are of the same order as the radius. For a winding much deeper than the former's radius, or a single layer on a long tube, it drifts; the single-layer form on the Wheeler page is better for the latter.
- Air core. The tube and the medium it carries are not in the inductance; a magnetised slurry raises it by about (1 + χ) of the medium's susceptibility, which the solenoid-field page carries.
- Copper at 20 °C. The resistance rises 0.39 % per degree, so a drive coil at 60 °C is 16 % higher than this.
- The 4 A/mm² ampacity is a rule of thumb for still air and continuous current — a figure to keep the enamel below its class temperature, not a limit the copper cares about. Pulses at a low duty can go several times higher; the current-rise page reports the pulse's resistive power so the two can be compared.
- Nothing here is Meyer's. The estate photographs show coils on tubes and dividers between them; no gauge, turn count or layer count is given anywhere the archive holds, and these are the numbers a reader would have to choose for themselves.