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Physics

Helical Coil Calculator

Enter your coil geometry to calculate inductance (Wheeler formula), coil height, total wire length, wire volume, resistance, magnetic field strength, stored energy, and resonant frequency. Switch between metric and imperial units at any time. The "show your work" panel walks through every formula with your actual numbers.

Your details

Outer-to-outer diameter of the winding measured at the coil centreline. In imperial mode, enter inches; in metric, millimetres.
mm
Diameter of the bare conductor (not including insulation).
mm
Total number of complete loops in the coil.
turns
Gap between adjacent turns, measured edge-to-edge. Set to 0 for a close-wound coil.
mm
DC or RMS current through the coil. Used to calculate magnetic field, stored energy, and time constant.
A
Distributed capacitance of the coil (self-capacitance). Used to compute the self-resonant frequency.
pF
Resistivity used to calculate DC wire resistance. Copper (1.724e-8 ohm*m) is the standard for most RF and power inductors.
Inductance (L)Low-frequency RF range
0.158uH

Single-layer inductance via Wheeler (1928) formula

Coil height (H)30
Wire length (Lw)1,885.19
Wire volume (V)1,480.628
DC resistance (R)0.0414ohm
Magnetic field (H)666.666A/m
Flux density (B)0.8378mT
Stored energy (E)0.079uJ
Time constant (tau)3.8182us
Resonant frequency126,615.54kHz
Coil height30.00 mm
Wire length1885.19 mm
Wire volume1480.628 mm³
Inductance (uH)0.158
Resistance (ohm)0.0414
Energy (uJ)0.079
00.160.3212140
Number of turns (N)

Inductance: 0.1580 uH

  • Inductance of 0.1580 uH falls in the low RF (0.1-10 uH) range.
  • DC resistance is 0.0414 ohm. Lower resistance means higher Q-factor and less power loss.
  • Self-resonant frequency is 126615.54 kHz. The coil behaves as an inductor only well below this frequency.
  • The L/R time constant is 3.82 us: the current rises to ~63 % of its final value in this time.
  • Axial flux density at the coil centre is 0.8378 mT (solenoid approximation, valid when coil height is comparable to or greater than diameter).

Next stepTo double the inductance, multiply the number of turns by sqrt(2) (about 28 turns), keeping the same geometry.

Formula

LμH=DcN218Dc+40Lw,H=N(Dw+S),Lw=N(πDc)2+(Dw+S)2L_{\mu H} = \dfrac{D_c N^2}{18 D_c + 40 L_w}, \quad H = N(D_w + S), \quad L_w = N\sqrt{(\pi D_c)^2 + (D_w+S)^2}

Worked example

A copper coil with 30 mm diameter, 1 mm wire, 20 turns, 0.5 mm spacing: Dc = 1.181 in, pitch = 0.0591 in, Lw = 76.5 in. L = (1.181 x 400) / (18 x 1.181 + 40 x 76.5) = 472.4 / 3081.2 = 0.153 uH.

What is a helical coil?

A helical coil is a conductor wound in a helix along a cylindrical axis. When current flows through it, the coil acts as an inductor: it stores energy in a magnetic field and opposes changes in current. The simplest and most common form is the single-layer air-core coil used throughout RF electronics, antenna matching networks, Tesla coils, and power supplies. The key geometric parameters are the coil diameter, the wire diameter, the number of turns, and the spacing between adjacent turns.

Wheeler formula for inductance

The inductance of a single-layer air-core coil is most commonly calculated with the Wheeler (1928) formula: L = (Dc * N^2) / (18 * Dc + 40 * Lw), where Dc is the coil diameter in inches, N is the number of turns, and Lw is the total wire length in inches. The result is in microhenries. Wheeler derived this empirical formula by curve-fitting to measured data; it is accurate to within about 1 % for coils where the length-to-diameter ratio is 0.4 or more. For shorter coils (length much smaller than diameter), Nagaoka coefficient corrections improve accuracy.

Wire length, height, and resistance

The axial height of the coil is H = N x (Dw + S), where Dw is the wire diameter and S is the gap between adjacent turns. The wire follows a helical path, so its true length per turn is sqrt((pi x Dc)^2 + (Dw + S)^2), not just pi x Dc. The extra term accounts for the axial advance per turn; it matters most for tightly spaced or thick-wire coils. The DC resistance is R = rho x Lw / A, where rho is the conductor resistivity in ohm-metres and A = pi x (Dw/2)^2 is the cross-sectional area. Resistance affects the Q-factor (Q = 2 x pi x f x L / R) and the L/R time constant.

Magnetic field, stored energy, and self-resonance

The axial magnetic field at the centre of the coil (solenoid approximation) is H = N x I / l, where l is the coil height and I is the current. The magnetic flux density is B = mu0 x H, where mu0 = 4 x pi x 10^-7 H/m. Energy stored in the inductor is E = 0.5 x L x I^2. The L/R time constant (tau = L/R) describes how quickly current builds up or decays. Every real coil also has a distributed self-capacitance C that forms a parallel LC resonator with the inductance; the self-resonant frequency is f = 1 / (2 x pi x sqrt(L x C)). Above this frequency, the coil behaves as a capacitor rather than an inductor.

Typical inductance ranges by application

ApplicationTypical inductance rangeFrequency range
VHF/UHF RF circuits1 - 100 nH100 MHz - 3 GHz
HF/shortwave radio (RF coils)0.1 - 10 uH3 - 30 MHz
Medium-wave AM radio50 - 500 uH500 kHz - 2 MHz
Tesla coil secondary10 - 100 mH50 - 500 kHz
Audio crossover filters0.1 - 10 mH20 Hz - 20 kHz
Power supply chokes10 uH - 10 mH10 kHz - 1 MHz

Air-core single-layer helical coils. Values are approximate; actual results depend on geometry.

Frequently asked questions

What is the Wheeler formula and when is it accurate?

The Wheeler (1928) formula calculates the inductance of a single-layer air-core coil as L (uH) = (Dc x N^2) / (18 x Dc + 40 x Lw), with Dc and Lw in inches. It is accurate to about 1 % for coils where the winding length is at least 40 % of the coil diameter. For pancake-style coils (length much less than diameter), accuracy degrades and Nagaoka or modified Wheeler corrections should be used.

How does the number of turns affect inductance?

Inductance scales roughly with N^2 for a fixed coil size, because both the number of flux linkages per ampere and the total flux increase with N. However, the Wheeler formula includes Lw (which also increases with N) in the denominator, so the actual scaling is slightly less than quadratic. To double the inductance, multiply turns by approximately sqrt(2) while keeping the geometry fixed.

What is the self-resonant frequency and why does it matter?

Every coil has distributed capacitance between adjacent turns. This parasitic capacitance (C) resonates with the inductance (L) at the self-resonant frequency (SRF) given by f = 1 / (2 x pi x sqrt(L x C)). Below the SRF the coil behaves as an inductor; above it the capacitive impedance dominates. For RF applications, you must choose a coil whose SRF is well above your operating frequency, typically by a factor of 3 to 10 or more.

How do I reduce the DC resistance of my coil?

DC resistance depends on wire material (copper is standard), wire diameter (larger diameter means lower resistance), and wire length. The most effective single change is to use thicker wire. A doubling of wire diameter reduces resistance by a factor of 4 (area scales as diameter squared). Switching from copper to silver reduces resistance by about 8 %, barely worth the cost except at very high frequencies. Litz wire can reduce AC resistance at high frequencies by mitigating skin and proximity effects.

What is the L/R time constant?

The time constant tau = L/R is the time it takes the current in the coil to reach about 63 % of its final value when a step voltage is applied (or to fall to about 37 % when the voltage is removed). It is the inductive equivalent of the RC time constant in capacitor circuits. A smaller resistance (better wire or thicker gauge) lengthens the time constant, while a smaller inductance shortens it.

How does spacing between turns change inductance?

Increasing the gap (S) between turns increases the coil height while keeping the diameter and number of turns fixed. A taller, more spread-out coil has a longer wire length (Lw), which enters the denominator of the Wheeler formula and reduces inductance. Close-wound coils (S = 0) give the highest inductance for a given number of turns and diameter, but also the highest self-capacitance due to closer turn proximity.

Sources

Written by Dr. Tomás Okafor, PhD Physicist · Lagos, Nigeria

Physicist specializing in classical mechanics, bringing 17 years of research and applied dynamics expertise to every calculator he reviews.

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