I've read that the cathodyne aka split load aka concertina phase inverter suffers from inability to adequately drive the output stage. I'm not sure this is really true ... at least for a 6V6 type amp like 5E3. ...
You got that 5E3, and you can turn up the volume enough to make the output tubes distort, right? Then obviously for this amp/example, the split-load has all the drive needed and then some...
I've read that the cathodyne aka split load aka concertina phase inverter suffers from inability to adequately drive the output stage. ... I've read in lots of places that the main disadvantage of Cathodyne is that it lacks drive for the output ...
Be careful to distinguish between "voltage gain" and "output voltage swing" when looking at phase inverter circuits. "Drive" is ill-defined and could be misinterpreted by readers (and maybe by writers).
No doubt about it, the split-load has a voltage gain which only approaches 1, so it has the least gain (by itself) of any of the phase inverter circuits. This could be what some mean when they say it lacks "drive". Practical split-load inverters are rarely used without additional gain stages before/after them, so this is somewhat immaterial in actual amps.
The split-load's challenge is that it needs to develop 2 output signals, moving in opposite directions, still leave voltage across the tube, and do all this from a single supply voltage. Whether it can do this well cannot be known without specifying the supply voltage for the split-load stage and the needed peak output voltage (or at least the bias voltage of the output tubes).
Any claim of whether the split-load can/can't drive the output stage is meaningless without knowing those two voltages. It
We'll use the
Princeton Reverb as an example.
The split-load supply voltage is 240v, and the needed peak output voltage (per output) is equal to the 6V6 bias voltage at 34v peak. So this means after the idle bias of the split-load is considered, it should be able to swing at least 34v in either direction, while still leaving voltage across the split-load's triode.
As biased, the split-load's plate is at 200v and its cathode is at 50v at idle. If a signal is applied to the split-load's grid which reduces current through the triode, the limit is for the plate to move to the B+ voltage and the cathode to move to ground voltage. Each can move 40-50v which satisfies the 34v peak output requirement in this direction.
What happens when the split-load triode draws more current, pulling the plate and cathode towards the same voltage? For the plate, 200v - 34v = 166v and for the cathode, 50v + 34v = 84v. This leaves 166v - 84v = 82v across the triode. That is likely a good amount of plate-to-cathode voltage to support the plate current needed to swing the outputs in this direction.
This last step (plate swinging negative, cathode swinging positive) is the portion of signal swing most likely to be a limiting factor with a split-load inverter. It is also the main spot you should be investigating to determine is the split-load has "enough drive". Hopefully you see why this can't be evaluated without knowing the supply voltage and output tube bias.
If you're working from a raw design, you'll need to start with the supply voltage & output tube bias then ask, "Will there be enough plate-to-cathode voltage (given my desired load resistors) when there is 4x the bias voltage subtracted from the supply voltage?" And then you need to subtract a bit more voltage to ensure the tube can swing the needed output without running into limits or linearity issues.
Returning to that Princeton, 34v * 4 = 136 and 240v - 136v = 104v. And from our ealier example, another 20v or so of available voltage is there as a buffer between the output requirement and tube capability.
You could also reality-check this by looking at a loadline for the Princeton's 12AX7 for 112kΩ (both 56kΩ loads are in series) and check that it will pass (240v - 82v)/112kΩ = 158v/112kΩ = 1.41mA at 82v on the plate at or below 0v on the grid.