A typical tube amplifier reacts with the loudspeaker load quite differently to a solid state amplifier - it puts extra power into the speaker at resonance and due to rising voice coil inductance at higher frequencies it puts out a progressively louder response as the frequency rises, solid state amplifiers do not do this and consequently lack the bottom end "balls" and top end "sizzle".
This little circuit aims to rectify that solid state amplifier "flat" sound - it is best used as the last effect in the chain before the solid state amplifier input socket, or in the effects loop etc. it can also be used directly in to a mixer or daw to give more tube amplifier type characteristics.
When the two spst switches are open the response is totally flat allowing the user to hear the difference when either the resonance or presence tone filters are bypassed - of course these can be separate toggle switches or a single dpst switch or even a footswitch - the choice is yours
When the switches are closed and both potentiometers are set to minimum, there is a slight boost at 100hz of about +2dB and a gradual rise from 1kHz to 10kHz of +3dB.
When both potentiometers are set to maximum, the resonant peak rises a further 4.5dB, and the presence rises a further 10dB. The resonance control should be a linear type and the presence a reverse log for the best operation contour - if you cannot find a reverse log pot then a linear will work, but most of the additional boost will be in the final 5 or so degrees of rotation.
The graphs show (both potentiometers) the full boost, minimum boost and flat conditions.
Enjoy and as always , your comments are most welcome.
cheers
bajaman
