Single Coil Inductance Calculator for Pickups

Single Coil Inductance Calculator

Estimate pickup inductance from turns, coil window area, winding length, magnetic core, wire gauge, DC resistance, cable capacitance, resonant peak and practical pickup voicing.

Named Pickup Presets
Coil And Circuit Inputs
Used for coil window width, height, depth and magnetic path length.
Area is the magnetic window cross-section used in the inductance estimate.
More turns increase inductance and resistance.
Accounts for scatter wind, taller layers and average turn length.
For an oval, this is the long axis across the bobbin.
For an oval, this is the short axis across the pole line.
Use when the coil footprint is irregular or already measured.
Approximate coil depth or magnetic circuit length through the winding.
Used with width and height to estimate average turn perimeter.
Sets an effective permeability estimate for pickup-scale geometry.
Gauge drives DC resistance and pack density estimates.
Resistance is corrected from 20 °C using copper temperature coefficient.
Include guitar cable plus pedal or amp input capacitance when known.
Layer count and insulation can shift this estimate.
Lower loads damp the resonant peak and darken the response.
Leave zero for tone wide open; add capacitance for darker settings.
This calculator uses the solenoid relation L = mu0 x effective mu x turns squared x area / path length, then applies pickup-specific empirical correction factors for fringing, winding build and magnetic cores.
Estimated Inductance
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henries
DC Resistance
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copper coil
Resonant Peak
--
with capacitance
Pickup Voice
--
voicing estimate

Calculation Breakdown

Pickup Spec Grid
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Coil window area
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Estimated wire length
--
Total capacitance
--
Damped Q estimate
Live Pickup Specification

Coil Geometry

Turns--
Window shape--
Area--
Path length--

Electrical Voice

Core factor--
Wire gauge--
Resonant peak--
Voicing--
Core And Magnet Reference Table
Magnet / Slug TypeEffective MuInductance EffectTypical Pickup VoiceUse In Calculator
Alnico 2 rods1.18Low-mediumSoft attack, sweet upper midsVintage neck and lower output bridge coils
Alnico 3 rods1.12LowClear, open, less pushEarly-style low pull single coils
Alnico 5 rods1.28MediumBright attack with firm lowsCommon Strat, Tele and bass single coils
Alnico 8 rods1.36Medium-highStrong output, tighter midsHot rod and higher drive single coils
Ceramic bar with steel poles1.90HighFocused, louder, more compressedBudget ceramic pickups and blade designs
Steel slugs or rail2.45Very highThick midrange and lower peakSingle-coil rails and steel slug conversions
Hybrid steel blade2.15HighEven string sensing, strong midsBlade pickups and narrow rail layouts
Air core reference1.00ReferenceWeak, experimental referenceTesting formula sensitivity only
Wire Gauge And Resistance Table
GaugeDiameter ApproxOhms Per 1000 ftTypical TurnsPickup Use
41 AWG0.071 mm10505500-7600Lower resistance, open custom coils
42 AWG0.063 mm16596500-9000Most vintage Strat, Tele and bass coils
43 AWG0.056 mm21437600-11000Tele neck, compact bobbins and hotter winds
44 AWG0.050 mm25938500-13000High turn count in tight coil windows
45 AWG0.045 mm33489000-15000Very compact high-resistance coils
Resonance And Voicing Table
Loaded Resonant PeakLikely VoiceCommon CauseAdjustment Direction
6.0 kHz and higherVery bright, glassy, lower outputLow inductance or low cable capacitanceAdd turns, use more cable pF or load lower
4.5 to 6.0 kHzClassic clear single-coil chimeModerate turns with Alnico rodsGood target for neck and middle coils
3.2 to 4.5 kHzBalanced, punchy, bridge friendlyMore turns, higher capacitance or stronger coreUseful for hotter bridge winds
2.2 to 3.2 kHzThick mids, P90-like weightHigh inductance or steel-assisted coreLower turns or cable pF for more openness
Below 2.2 kHzDark, compressed, heavy mid focusLarge inductance plus high capacitanceReduce tone capacitance or load less heavily
Preset Comparison Table
PresetTurnsCoreWireDesign Goal
Strat Neck Glass7600Alnico 5 rods42 AWGClear top with familiar vintage output
Tele Bridge Bite8200Alnico 5 rods43 AWGSharper bridge edge with extra resistance
P90 Soapbar Thick9800Alnico 2 with broad coil42 AWGHigher inductance, wider coil aperture
Jazz Bass Round8500Alnico 5 rods42 AWGRound bass response with usable top
Steel Slug Rail9000Steel rail / slugs43 AWGHigh inductance and stronger mid focus
Tip 1: Measure the actual coil window and winding depth on the bobbin. A small area or path-length error changes inductance more than most players expect.
Tip 2: Cable capacitance is part of the pickup voice. The same coil can sound bright through a short low-pF cable and darker through a long high-pF cable.

Before you play a single note, the world opens or closes with that very first sound you hear when you plug in your guitar. That instant tonal snapshot are neither magic nor physics; it’s caused by copper wire wrapped around bar of magnetic steel. Before you even pluck a string, the connection settles into place and do battle with resistance of your amp and the capacitance of your cable.

Players most often believe that their tone stem from pickups or even the wood they are made from. But it isn’t. There is something more electrical going on here. And this is where single coil inductance calculator steps in. It takes raw geometry and turns it into audible character. This means no one has to guess what will happen if you wrap some extra wire around a magnet or use a different one.

Why Inductance Changes Your Guitar Tone

What does all that mean? Well, basicly, it’s just how much your pick up resists a change of current, aka inductance. In turn, that means directly how your pick up cuts through the mix. For instance, if something has high inductance it will soften its attack and thicken the low end by pushing resonant peak down. If something has low inductance, then it stays pretty glassy and bright.

Compare the difference between a P90 soapbar pickup and a standard Stratocaster neck pickup. A Strat usually runs about seven thousand turns with moderate inductance resulting in articulate chime. A P90 often pushes ten thousand turns. That raise the inductance enough to drop the peak frequency and add some weight to the mids. And neither is better than the other. They’re aimed at different parts of sound range. It helps you know where your setup sit. It can also help you decide if you want more output or something else.

But it’s not only about the number of turns of wire; it’s also about the core material. Most vintage guys will know exactly what I’m talking about. A good alnico 5 rod offer a solid, crisp starting point. Move to a high-permeability ceramic bar or steel slug and magnetism clamps down on the field tighter. You’ve increased the inductance without adding any extra turns of wire, which moves the voice towards a more compressed, heavy sound. Because the calculator take these material differences into account, it displays them in its permeability factor. In this way, it illustrates how something as simple as changing your core can have the same effect as rewinding completely.

Little things matter a lot when you’re chasing after that special sound while trying not to break the bank with purchases. The length of the cable also has an effect on the high end that we often don’t think about unless we connect it to our pedalboard. Each foot of cable create capacitance. This interacts with the pickup’s inductance to create a low-pass filter. With a short six-foot cable, your resonant peak is left wide open. Those crisp upper harmonics is preserved. When you run twenty feet of cheap coax out to the back of the stage, that peak gets pulled down into the mud. By entering your estimated load in picoFarads (pF), the tool models this drag and shows you just how much brightness you’re losing before signal reaches the first pedal. This sheds some light on what makes a bright pickup sound dark in a live setting. And it could of help you compensate for this by picking a lower-capacitance cable or playing with your tone pot at home.

Another thing to think about is the effect that wire gauge have on the relationship between DC resistance and inductance. The thinner the wire (such as 43 AWG), the smaller the diameter, which gives you more turns per unit of space, increasing both resistance and inductance. The thicker the wire (41 AWG), the lower the resistance, though this also reduce the amount of inductance that can be packed into a given space. Here’s the rub: Inductors with higher resistances is warmer. But when run through an overdriven amplifier, they compress signal at a quicker rate. In contrast, lower resistance coils respond better to picking dynamics while feeling open and lively. It is all a matter of balance.

Sometimes chasing high output come at the cost of some clarity. Capacitive load, electrical resistance, magnetic field strength all play into tone: it’s a balancing act. You can’t optimize for one thing while optimizing for another. Pursue thick lows and you’ll probably sacrifice some high-end. Go after sparkling brightness, and you will have a thin dynamic range that doesn’t hold together well when mixed with other bands.

Your ears determine what works; the calculator gives you the numbers. Experiment with its limits on your existing equipment. Then, take a step back and listen: where does the music liv? Where’s that first note telling the truth? As long as you learn how to ask the question the right way, the answer is always there.

Single Coil Inductance Calculator for Pickups

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