The Valve Wizard

How to design guitar effects!

Spark Gap 2: Low Voltage Valve Overdrive

Most guitar overdrive effects rely on diode clipping to generate distortion, and many players like to experiment with different kinds of diode, Zeners, and LEDs. Some also experiment with valve diodes in an attempt to emulate the sound of an overdriven valve amplifier. However, at low voltages the results are often disappointing, because a valve diode will normally conduct some forward current even when the voltage across it is zero or slightly negative (this current is driven by the space charge itself). For very small signals, a valve diode therefore looks more like a resistor than a diode, producing a weak distortion sound at best.

However, some years ago I discovered something interesting about the EB91/6AL5 –a very common and cheap double diode. When its heater voltage is reduced, its whole I/V characteristic shifts to the right, creating a useful diode characteristic for small signals, as illustrated in the graph further down this page. Most other valves do not behave this way, their dynamic resistance simply increases when the heater voltage is reduced, without changing the actual diode threshold voltage. I exploited this property of the EB91 to create a kind of Tube Screamer with real valve diodes, which I called Spark Gap. However, my original design was pretty basic -just a proof of concept- and it could only acheive mild overdrive. Finally I re-visited the idea and present here "Spark Gap 2", the first distortion pedal I am actually proud of. Unlike it's wimpy predecessor it can acheive high levels of creamy to crisp, true-valve overdrive, and a huge tonal palatte, with surprisingly few parts. Best of all, it does not suffer from the 'woolly', flatulent overdrive quality of most other low-voltage tube pedals.


Since effects pedals normally operate from a 9V supply, two valves were used with their heaters in series, so each operates at 4.5V. The junction of the two heaters also provides a convenient half-rail voltage –filtered by R13 and C13– for biasing the opamps. R12 and C14 provide additional filtering for the opamp’s supply rail, and D1 provides polarity protection for the opamp.


U1a buffers the incoming guitar signal as well as providing adjustable gain. C2 and C3 progressively narrow the bandwidth as the gain is increased, to reduce ‘muddiness’ at the low end and shrillness at the high end. U1b serves as a second buffer and final tone control, tuned to produce a mid hump or scoop around 800Hz, which I found worked best for me.

Since the dynamic resistance of the valves is relatively high, two stages of diode clipping are cascaded between the two opamps, so a high level of distortion can be achieved. C5 and C6 provide additional filtering of excessively shrill harmonics. With SW1 closed, both clipping stages are symmetrical, which mimics the symmetrical clipping of a purely push-pull amplifier, and the final result is similar to most diode-clipping pedals on the market. But there is one final trick to be played here.

When SW1 is open, the first clipping stage becomes asymmetrical. C4 is now able to charge rapidly through R6+V1 on positive cycles, but it can only discharge more slowly through R6+R7+V2 on negative cycles. This causes the average voltage across V1 to shift negatively during overdrive, which dynamically changes the clipping threshold depending on the signal amplitude. Exactly the same effect occurs in most real valve amplifiers. It causes the overdrive sound to change or ‘swirl’ as the guitar signal sustains and decays, and it allows the player to exploit different tones by varying how hard s/he plays, ‘riding’ the clipping threshold as it were. This is something most commercial distortion pedals do not do, leading them to sound rather monotonous compared to a real amplifier.


MOSFET Q1 is the familiar Millennium bypass circuit, for click-free switching of the status LEDs, allowing a DPDT footswitch to be used for bypassing the effect. I mounted the LEDs underneath the valves so they light up when the effect is active. Total current consumption is about 260mA, depending on valve heater tolerance. This is relatively high for a pedal, so battery power is out of the question. It is essential to use a good quality, quiet power supply, which is often the price that is paid for using valves, but well worth it in my opinion.

The whole circuit is squeezed onto a slim PCB, and the valves poke out the side of the enclosure (if you can't see the valves it doesn't sound as good, right?). The PCB is held in place mainly by the pots (since they mount to the enclosure), and the DC input jack and enclosure lid lock it in place further, making a simple but firm assembly. I built this for my own personal use; if it was made for regular gigging it would probably benefit from a different arrangement with more protection for the valves, of course.