... where would you bias my amp? It's 2X6V6 JJ's with a marshall style PI and the OT is a custom made 4K (which is low for 6V6 i think?) 30 watt heyboer with only 8 and 16 ohm taps. So as i understand it, the ideal load would be a 16 ohm speaker off the 8 ohm tap but my speaker is 8 ohm so i'm runnning that off the 8 ohm tap. ...
4kΩ and 30w sounds typical for a pair of 6L6's (or 4x 6V6's) at typical guitar amp voltages. It probably wouldn't be optimum for
maximum clean output power from a pair of 6V6's, but also likely does no harm.
I'd set the bias to 70%.
Even with that OT, and why? (just curious)
The below recently occurred to me; I've never read anyone explain the "70% rule" as I will below, but it might be out there somewhere.
Class A is 100% dissipation at idle, and presumes the supply voltage and OT load are such that the output tube(s) will swing from idle current to 2x idle current, back to idle and down to (almost) zero current and back to idle. At no point in the maximum clean output signal cycle does the tube shut off.
Class B (theoretically) idles at 0% dissipation, just turned off. Since the tube is cooling (off) exactly half the max output signal cycle, much bigger plate voltage and current swings are permissible, for much more power output. This requires the supply voltage and load to be sized accordingly. It also assumes the two half-cycles generated by the push-pull output stage can be stitched together perfectly to create a unified output.
Class AB is literally anything between Class A (100%) and Class B (0%). The designer can tweak in the bias to be exactly where they (think they) want, based on their supply voltage, OT load, and expected plate dissipation throughout the signal cycle. Where they think they want it is necessarily based on some assumed ideal tube.
In the real-world, that last statement on Class B is tough to achieve. Class AB which is operating very cool (closer to Class B than Class A) may sound rough due to crossover distortion and incomplete "stitching together" of the signal. Class AB conditions (high supply voltage, very low OT load) can overheat the tubes if they're idling too close to Class A.
Look at a "
Unit Circle" (a foundation for discussing sine waves). The midpoint between a sine wave at 0 degrees (zero, off, or reference point) and its positive peak at 90 degrees is at 45 degrees. The distance in the Y-direction hasn't rising to 50% of the peak, but is actually at 70.7%, 1/√2, √2/2 or sin45-degrees (all basically the same number). This is also the percentage used to convert an sine wave's peak to its RMS value to express what value of d.c. would have an equivalent heating effect (same amount of power over time).
The "new idea" (I'm probably just now recognizing the "old idea") is that idling at ~70% is the same as "halfway between Class A and Class B, when the output stage is driven by sine waves" (as it often is in testing).
So just try 70% dissipation as an idle point. Ass PRR says, if it sounds too rough with small signals, idle a little hotter; if it tends to redplate when pushed hard, idle a little cooler.