IMO "current" gets overstated when talking about phase inverters.
Yes well, even the Silverface amps weren't optimum scientific designs. A 47k plate load ... with each 12AT7 triode ... the load line looks better (in terms of output swing) than a 12AX7 under similar circumstances.
Certainly!
On one hand, same-supply-voltage with smaller-plate-resistance & using a tube-with-lower-internal-resistance all amounts to "more current." That's Ohm's Law at work.
But novices read "more current" and think the phase inverter is delivering current into the output tube grids, which I showed earlier it is entirely incapable of doing. Other errors build on the logic of assuming that's the case, and eventually they have a bit to un-learn if they wish to advance their knowledge.
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A more helpful way of thinking of the issue is focusing on Resistance, not Current.
As I said before I think Fender chose 68kΩ grid-leak resistors, then made follow-on decisions to support that choice. In picking a plate load resistor for the phase inverter, the common rule of thumb is the grid-leak should be 2-5x the plate load resistance (RDH4, Page 482).
For onlookers, the grid-leak is in parallel with the plate load for AC signals.
For grid-leak 2x the plate load resistance, the effective load is 67% of the plate load resistor value.
For grid-leak 5x the plate load resistance, the effective load is 83% of the plate load resistor value.
For grid-leak 10x the plate load resistance, the effective load is 91% of the plate load resistor value.
So for 68kΩ we would be thinking 34kΩ (or the standard-value of 33kΩ), though Fender chose a bit higher at 47kΩ.
In the same way, we would like the plate load resistor to be 2-5x the tube's internal plate resistance. That's because this internal resistance forms a voltage-divider with the plate load resistor, so lower internal resistance means the tube's in-circuit gain is a bigger % of Amplification Factor.
We have a plate load of 47kΩ, so we would really like the tube's internal plate resistance to be down to 23kΩ (1/2), or even as low as 10kΩ (1/5).
Using the graph on Page 4 of the
12AT7 data sheet, we can estimate the internal plate resistance.
Schematic figures imply ~2.7mA per triode, so I drew a Red vertical line at 2.7mA.
Schematic says 245v plate & 120v cathode, so I follow the vertical up to the intersection with the Rp curve for "100v plate"
Reading the value at the left, the 12AT7 has about 17.5kΩ of internal plate resistance.
Turns out, we're reasonably close to the plate load resistor being 3x the internal plate resistance (a good pairing). With a Mu of 60, we anticipate a basic gain of around 60 x (47kΩ/(47kΩ + 17.5kΩ)) = 43.7 (actual gain in a long-tail is much lower due to feedback across the tail resistance).
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So we see that thinking in terms of "bridging resistance" (where load resistance is much bigger than source resistance) is an easier rule to apply. It also betters support logical intuition, and makes for easier back-of-envelope calculations when we consider that amps are typically designed from the output backwards towards the input.
(I had to "waste" a lot of time un-learning bad amp electronics info, and unhelpful concepts. That's why I keep pushing what I believe to be the more-useful ways of conceptualizing amp circuits)