Gibson Les Paul volume and tone
A guitar’s pickups, switch, volume and tone, with the cable and amp input, solved part by part. Flip the switch, split a coil, turn the knobs and watch the curve. Pin a setting to compare, change any part, and listen.
Two humbuckers, each with its own 500 kΩ volume and tone pots and a 22 nF cap, joined at the 3-way switch after the volume pots. In the middle position you see each pickup’s share as well as their sum.
Swipe sideways for the whole drawing. Tap a part to change it. The pickups are on the left, and the cable and the amp input hang on the right.
At this setting
0 dB is the pickup’s raw voltage, before the coil, knobs, cable and amp input shape it. The peak up top is the pickup’s resonance.
Pin this curve keeps what the graph shows, up to three pins in their own colors. Pins stay when you switch guitars, so you can lay a Strat’s neck pickup over a Les Paul’s. In a sweep, the lightest line is the knob at 0 and the darkest is 10.
Listen
The amp input
Driven by
What the cable plugs into
The knobs
- Neck volume
- Works in the neck and both positions. With both pickups on, it also sets how hard the neck side loads the bridge pickup, and at zero it mutes the guitar.
- Bridge volume
- The same for the bridge side.
- Neck tone
- Turned down, the neck cap sits across the neck pickup and the peak moves down.
- Bridge tone
- The same for the bridge pickup.
Switch positions
- Neck
- The neck pickup with its volume and tone. The bridge side is disconnected.
- Both
- Both volume wipers tie together at the switch. Now each volume pot loads the other pickup too, and turning either volume to zero mutes both.
- Bridge
- The bridge pickup with its volume and tone.
Coil modes
- Series
- Both coils in series, the way the pickup is normally wired.
- Parallel
- Both coils in parallel, in phase. The pickup’s inductance and resistance drop to about a quarter, so its resonant peak moves up and its output drops.
- Screw coil
- The screw coil alone, with the slug coil shorted, as a coil-split switch does it. The shorted coil still sits next to the live one and pulls a little current through their coupling.
- Slug coil
- The slug coil alone, with the screw coil shorted. Which coil stays live in a split depends on how the pickup and the switch are wired.
Parts
- Neck screw
- The neck pickup’s screw coil voltage, from the string moving in the magnet’s field near the neck. It’s half the pickup’s voltage, since the two coils are assumed to have equal turns.
- Screw R
- 4.5 kΩ, The screw coil’s resistance, measured alone on a PAF-style humbucker (screw coil 4.5 kΩ, slug coil 4.2 kΩ).
- Screw L
- 2.67 H, The screw coil’s inductance, measured alone at 1 kHz (screw coil 2.675 H, slug coil 2.56 H).
- Neck slug
- The neck pickup’s slug coil voltage, from the string moving in the magnet’s field near the neck. It’s half the pickup’s voltage, since the two coils are assumed to have equal turns.
- Slug R
- 4.2 kΩ, The slug coil’s resistance, measured alone on a PAF-style humbucker (screw coil 4.5 kΩ, slug coil 4.2 kΩ).
- Slug L
- 2.56 H, The slug coil’s inductance, measured alone at 1 kHz (screw coil 2.675 H, slug coil 2.56 H).
- Coupling
- k 0.127, How strongly the two coils share their magnetic field, entered as k (0 is none, 1 is complete). Measured alone, the two coils add up to 5.235 H, and the pickup in series reads 5.9 H. So each coil adds M = 0.33 H to the other, and k = M / √(L1 L2) = 0.127.
- Winding C
- 140 pF, The capacitance between the neck pickup’s turns, across its output. A typical figure, not a measurement. It stays the same whichever coils are on.
- Bridge screw
- The bridge pickup’s screw coil voltage, from the string moving in the magnet’s field near the bridge. It’s half the pickup’s voltage, since the two coils are assumed to have equal turns.
- Screw R
- 4.5 kΩ, The screw coil’s resistance, measured alone on a PAF-style humbucker (screw coil 4.5 kΩ, slug coil 4.2 kΩ).
- Screw L
- 2.67 H, The screw coil’s inductance, measured alone at 1 kHz (screw coil 2.675 H, slug coil 2.56 H).
- Bridge slug
- The bridge pickup’s slug coil voltage, from the string moving in the magnet’s field near the bridge. It’s half the pickup’s voltage, since the two coils are assumed to have equal turns.
- Slug R
- 4.2 kΩ, The slug coil’s resistance, measured alone on a PAF-style humbucker (screw coil 4.5 kΩ, slug coil 4.2 kΩ).
- Slug L
- 2.56 H, The slug coil’s inductance, measured alone at 1 kHz (screw coil 2.675 H, slug coil 2.56 H).
- Coupling
- k 0.127, How strongly the two coils share their magnetic field, entered as k (0 is none, 1 is complete). Measured alone, the two coils add up to 5.235 H, and the pickup in series reads 5.9 H. So each coil adds M = 0.33 H to the other, and k = M / √(L1 L2) = 0.127.
- Winding C
- 140 pF, The capacitance between the bridge pickup’s turns, across its output. A typical figure, not a measurement. It stays the same whichever coils are on.
- Neck vol
- 500 kΩ, Neck volume, 500 kΩ audio taper. Its wiper goes to the switch, so with both pickups on, turning it to zero grounds the output and mutes both.
- Neck tone
- 500 kΩ, Neck tone, 500 kΩ audio taper, used as a variable resistor in series with its cap.
- Tone cap
- 22 nF, The neck tone cap.
- Bleed cap
- 1 nF, Treble bleed cap across the neck volume pot’s top half. It keeps the treble as the volume comes down.
- Bleed R
- 150 kΩ, Sits in parallel with the bleed cap so the treble lift doesn’t get too big at low volume settings.
- Bridge vol
- 500 kΩ, Bridge volume, 500 kΩ audio taper. Its wiper goes to the switch, so with both pickups on, turning it to zero grounds the output and mutes both.
- Bridge tone
- 500 kΩ, Bridge tone, 500 kΩ audio taper, used as a variable resistor in series with its cap.
- Tone cap
- 22 nF, The bridge tone cap.
- Bleed cap
- 1 nF, Treble bleed cap across the bridge volume pot’s top half. It keeps the treble as the volume comes down.
- Bleed R
- 150 kΩ, Sits in parallel with the bleed cap so the treble lift doesn’t get too big at low volume settings.
Pickups and load
Each humbucker is two coupled coils, each with its own measured resistance and inductance and half the pickup’s voltage. Both pickups use the same values. The coil buttons switch between series (as built), parallel, or one coil by itself. With 1950s wiring on, each tone control hangs off its volume’s wiper, so turning a volume down cuts less treble. With two pickups on, each one loads the other through its coil. Without the string model, the graph adds them as if their voltages were equal and in phase. On a real string each harmonic reaches the two pickups at a different strength and sign, and that’s what makes the in-between positions sound the way they do. The string model uses a 24.56 in scale, with the pole rows measured from the bridge saddle at about neck 5.51 and 6.2 in, bridge 1.3 and 1.99 in (measured by Swell Amplification to the visible pole row of each covered humbucker, approximate, with the other row 17.5 mm away). Harmonic n reaches a pickup x from the saddle scaled by sin(nπx/L), with L the string length, so a pickup near a node barely picks that harmonic up, and two pickups can cancel it. Each humbucker counts as its two pole rows, half its voltage each, which cancels the harmonics whose wavelength on the string is twice the row spacing. The string is ideal and each pole row is a point under it (a real pickup’s wider window softens the top harmonics). Saddle intonation is left out. The treble bleed option puts 1 nF in parallel with 150 kΩ across the top half of each volume pot. Other values are common too, and you can change both. The cable is about 15 feet (450 pF) into a 1 MΩ amp input.
Warnings. The summary above the graph turns red if the guitar can’t be solved as set, usually from a part at zero or a shorted pot track.
How this tool works. We solve each guitar with the circuit bench’s engine at 161 frequencies from 20 Hz to 20 kHz, cable and amp input included. Each pickup is a voltage behind its coil’s resistance, inductance and winding capacitance, and a humbucker is two coupled coils. With several pickups on, each one’s share is solved with the others shorted, and the shares add up.
The curves are linear. They leave out the pickup’s magnetic nonlinearity, the width of string under it, and the body and neck. The played string has the first two. Coil values are measured where a part’s description says so, typical otherwise. For an amp’s tone stack, try the tone stack and filter tool. To play a guitar into a whole pedal or amp, use the circuit bench.
Spot an error, or want a circuit added? Email info@swellamps.com. A schematic or a clear photo of one helps. Anything you send may be used to improve these models and our desktop app.
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