Air-Core Inductor Calculator
Estimate inductance of a single-layer air-core solenoid from coil geometry (turns, diameter, length) using Wheeler's formula.
How to Use
- Enter number of turns, coil diameter, and coil length.
- Uses Wheeler's formula for single-layer solenoids.
- Result is in µH; accurate to ~5% for coils where length is similar to diameter.
Show Work
Formulas
History of Wheeler's Formula
Harold A. Wheeler published his famous approximation for single-layer solenoid inductance in 1928 while working at the Hazeltine Corporation. Wheeler was a prodigy — he had already designed an automatic volume control circuit that Hazeltine licensed widely — and his single-line formula replaced laborious tables of elliptic integrals that radio engineers had been wrestling with since Maxwell and Nagaoka. His paper "Simple Inductance Formulas for Radio Coils" in the IRE Proceedings gave ±1% accuracy across the practical range of radio-era coil geometries and is still the starting point taught today.
The underlying physics goes back to Ampère's 1820s experiments on magnetic fields from current-carrying coils, then to James Clerk Maxwell's mathematical treatment in his 1873 Treatise on Electricity and Magnetism, and to Hidetsugu Nagaoka's correction factors for finite-length solenoids published in 1909. Wheeler's contribution was practical: distilling decades of pure-physics results into a calculator-friendly formula a radio engineer could use in the lab without a table.
Air-core coils remain the go-to choice for RF work — they have no saturation, no frequency-dependent core loss, and perfectly linear L-versus-current behavior. Most HF matching networks, tank circuits, and antenna traps still use hand-wound air solenoids designed with Wheeler's formula nearly a century after he published it.
About This Calculator
Enter the number of turns, coil diameter, and coil length. The calculator applies Wheeler's metric-unit formula and returns inductance in microhenries, plus the total wire needed to wind the coil and the turn density. For tightly wound coils (length similar to diameter, like most RF tank circuits), accuracy is within 1%; very short or very long coils stray further and you'd need a finite-element EM solver for high precision.
This tool assumes a single-layer, close-wound air-core solenoid on a non-magnetic former. For multi-layer coils, toroidal windings, or cores with ferrite or powdered-iron material, the formulas change — use the appropriate core datasheet's AL factor instead. Everything here runs client-side; no values leave your browser.
Frequently Asked Questions
What is Wheeler's formula?
Empirical approximation: L(µH) = (r²·N²) / (9r + 10ℓ), where r is radius and ℓ is length in inches. Accurate to 1% when ℓ > 0.4r.
Air-core vs ferrite?
Air-core: linear, no saturation, lower inductance per turn. Ferrite/powdered iron: much higher L in the same space but saturates at high currents and has frequency-dependent loss.
For RF applications?
Air-core coils are preferred for RF because ferrite cores lose effectiveness at high frequencies. Hand-wound air solenoids are common in HF-UHF filters and matching networks.
Common Use Cases
RF Tank Circuit
Hand-wound coil for an LC oscillator at 10 MHz — calculate turns/diameter to hit target L.
Radio Antenna Matching
Loading coil for short antenna — size it to resonate with capacitor at target band.
EMI Choke
Ferrite-core choke uses different math, but air-core Wheeler is the starting point.
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