Calculate inductance of single-layer and multi-layer solenoid coils. Determine turns, wire gauge, impedance, and resonant frequency for coil design.
The Coil Inductance Calculator estimates air-core solenoid inductance using Wheeler's formulas. It is meant for the common coil-design problems that come up when you are choosing a form, estimating turns, or checking whether a target inductance is realistic. It gives you a practical first-pass estimate before you start winding wire or refining an RF design. That is especially useful when small geometry changes can save a failed prototype winding.
It works for single-layer and multi-layer coils, and it can also solve for turns when you already know the inductance you want. That makes it useful both for forward design and for reverse-checking a planned winding.
Enter coil diameter, length, turns, and an optional capacitance value to see inductance, reactance, impedance, and resonant frequency. The calculator is especially helpful when comparing a few candidate geometries before you wind the coil or order parts. It gives you a quick check before you cut wire or commit to a former. That is useful when you want to know whether the coil will land in the target range before winding starts.
Use this calculator for a quick air-core inductance estimate or to compare turns, diameter, and length before winding a coil. It is useful for RF work, filters, and design checks, especially when you want to see how geometry changes affect the result. That helps you avoid winding a trial coil blindly when a geometry check would answer the question first.
Single-Layer (Wheeler): L (µH) = (d² × N²) / (18d + 40l). Multi-Layer (Wheeler): L (µH) = (31.6 × N² × r²) / (6r + 9l + 10c). Where d = diameter (inches), l = length (inches), N = turns, r = mean radius (inches), c = winding depth (inches). Reactance: X_L = 2πfL. Resonant Frequency: f₀ = 1 / (2π√(LC)).
Result: 25.5 µH
L = (1² × 50²) / (18×1 + 40×2) = 2500/98 = 25.5 µH (Wheeler formula). At 1 MHz: X_L = 2π × 10⁶ × 25.5×10⁻⁶ = 160 Ω.
Harold Wheeler published his famous inductance formulas in 1928. The single-layer formula L = d²N²/(18d+40l) (in inches and µH) remains the standard quick calculation method. Its simplicity and reasonable accuracy (±1% for practical coils) have kept it in use for nearly a century.
For metric units: L(µH) = (d_cm² × N²) / (45.72×d_cm + 101.6×l_cm). Or convert to inches first. The formula assumes uniform turn spacing and no magnetic core.
The quality factor Q = X_L/R_DC (at a given frequency) measures how close the coil is to an ideal inductor. Higher Q means lower losses. Typical air-core coil Q values: 50-300 at RF frequencies. Q is maximized when the length-to-diameter ratio (l/d) is approximately 0.45 for a single-layer coil, and when wire diameter is about 60% of the turn spacing.
Single-layer solenoid coils are used in radio tuning circuits, antenna matching networks, RF filters, Tesla coils, crystal radio receivers, and educational demonstrations. Multi-layer coils appear in power supply filtering, speaker crossovers, relay solenoids, and electromagnetic experiments. The design equations in this calculator apply directly to these applications when air-core or known-permeability cores are used.
Wheeler's formula is a practical engineering approximation, not a perfect physical model. It is usually very good for ordinary air-core coils with sensible proportions, but accuracy drops for very short coils, coils with unusual spacing, or cases where the geometry is far from the assumptions behind the formula. If you need tighter precision, compare against measurements or a more specialized model.
Single-layer coils wind all turns in one layer, which keeps the geometry simpler and usually lowers parasitic capacitance. Multi-layer coils stack turns in more than one layer, which can fit more inductance into less space but also makes the electrical behavior less ideal. The choice is usually a tradeoff between simplicity, size, and frequency performance.
Yes, very strongly. This calculator assumes an air core with relative permeability near 1, so it gives the baseline inductance for the geometry alone. Ferrite and iron powder materials can raise inductance dramatically, but the exact increase depends on the material type, core shape, and operating frequency. If you add a magnetic core, the air-core result should be treated as a starting point only.
Keep the winding single-layer when possible, space turns consistently, and avoid overlapping wire paths. Using a form with lower dielectric loss and choosing an appropriate wire size also helps. Lower parasitic capacitance pushes the self-resonant frequency higher, which matters most for RF and broadband designs.
The right gauge depends on current, frequency, and the amount of heating you can tolerate. Thin wire is fine for small-signal or experimental coils, but power inductors need thicker wire to keep resistance low and prevent excessive temperature rise. At higher frequencies, skin effect becomes important, so Litz wire can be a better choice than a single solid conductor.
Self-resonant frequency is the point where the coil's inductance and parasitic capacitance resonate together. Below that frequency the coil behaves like an inductor, but above it the behavior changes and the part no longer looks like a clean inductor. In practice, you want to operate comfortably below SRF so the coil stays stable and predictable.