For the non inverting (feedback) input, I can see how reducing its cap value would help with bias shift / blocking distortion for the given scenario. But can’t see how a grid stopper would help there? ie as it’s decoupled to (near enough) circuit common, how can the grid’s potential get pulled up above its cathode, (which would be necessary for grid current to flow and hence a grid stopper be beneficial)?
Aren't you acknowledging grid current when you agree that reducing its cap value would help with bias shift/blocking distortion? Where does the current come from that charges this cap for grid shift/blocking distortion?...
My thinking is that when overdriven, the dc operating point may shift around a bit. Long time constants at the grid will tend to slow down its ability to keep up with those changes.
...You don't think that the connected cathodes can swing far enough negative to make the non-inverting grid-to-cathode voltage positive?
Haha, I'm having a hard time getting my head around it, with that triode operating in common grid mode and the dc elevation.
It would be nice to get it on the scope, but as I don't have a galvanic isolation transformer for it, I suspect that without that, the scope inputs would load the circuit too much.
The LTP cathode of an overdriven in a JTM45 type circuit can certainly respond to the signal, Vp-p there looks about 5V. I think that if I add a grid stopper to the non-inverting section's grid, eg 10k, grid current would manifest as VDC appearing across it, when the signal exceeds a certain level. Does that sound right? If so, I'll try to check it out.