Thanks for pointing me to that! I hadn't realized the cathode follower was biased so close to the 0v grid line.
But the example is also a little bit out of context. Let's place it in the context of a 5F6-A Bassman.
Due to the nature of a cathode follower, you need to ignore the size of the input signal somewhat when you look at the follower's loadline. Instead, know that the gain will be somewhat less than 1, so focus instead on the
output signal, as implied by the plate voltage axis. For Merlin's example, as we move along the loadline to 0v on the grid, the plate voltage (and as he says, really the cathode-to-ground voltage) indicated is ~205v. The idle point appears to be at about 195v, so the cathode follower can output a 10v peak signal (or 20v peak-to-peak, as Merlin uses for his test).
Merlin's example assumed a 300v supply and 195v grid and cathode-to-ground. But the
5F6-A Bassman schematic indicates a 325v supply and 180v cathode-to-ground. This means for us that the operating point is shifted down and to the right along the loadline Merlin presented, which allows for more headroom from the follower.
I won't redraw these lines here, because Richard Kuehnel has published a
fairly exhaustive analysis of the 5F6-A Bassman, and I will make use of the conclusions he presented. The follower's operating point is still pretty close to the 0v grid line, but his analysis showed a headroom of 37.2v peak (as opposed to Merlin's example with 10v peak headroom).
Now, let's step backward from the output tubes. The schematic shows the bias is -48v. In the same way that we get compression and distortion as we approach and exceed the 0v grid line on the cathode follower's loadline, we will distort the output tubes heavily if we drive them beyond 0v on the grid. Since the bias is -48v, we can apply a positive 48v peak signal to drive the output tube grids momentarily to 0v. That will be our reference point as we work backwards through the amp.
The long-tail inverter is a handful to analyze. A simple rule-of-thumb for figuring on a napkin is that the gain to each output of the long-tail will be about 1/2 the gain one would expect from the tube used as a typical common-cathode gain stage. So if we might normally expect a gain of 52 from a 12AX7 stage, we could expect a gain of roughly 52/2 = 26 from a single output. In truth, the feedback loop reduces this gain somewhat. The gain from each half of the long-tail is also slightly different. The math is a handful to say the least, but Kuehnel found that the gains to be 25 and 26.6 before feedback, and 21.9 and 22.6 after feedback.
From this, an input of 48/21.9 = 2.19v peak will drive the output tubes to significant distortion. I used the lower gain number for the inverter, as it requires more signal from the cathode follower.
The tone stack is an issue. The only time you get a "flat" response (where loss is equal at all frequencies) is when the Mid pot is at maximum, and the other pots are at a minimum. So we oughta select something reasonable as a reference, and realize we will get more and less signal throughput at other settings. Let's work from all controls at half. I used Duncan's tonestack calculator, and plugged in Kuehnel's findings for cathode follower output impedance (531 ohms) and long-tail input impedance (1.9M, worst case), as well as 5F6-A parts values. The midrange dip represents the most loss under these conditions, and therefore the point at which the cathode follower has to supply the most signal to still drive the output tubes to 0v. The loss at the mid-dip with all controls at half is almost -13dB.