however, it is likely why big Class AB amps have chokes feeding their screen power supply node.
I'd think another reason would be economy: feeding the screen supply rather than the plates/whole b+ rail requires significantly less current capability and one less filter capacitor
True, High-Current Many-H chokes are big and expensive. Many have said over the years that once upon a time iron & copper were cheap, but many-µFs in a reasonably-small space were expensive. Back then, iron instead of capacitors (or electronic regulators) was how filtering got done.
But chokes tend to
choke or fight big changes of current. While you can filter the entire B+ supply of a Class AB amp, you're gonna need many-many-µFs in the filter cap after the choke & at the OT/plate node. Class AB amps have very large changes of plate current, which is part of what makes them AB (people focus too much on the biasing).
But Class AB is push-pull: The voltage-output that
would have occurred due to ripple fed to the center-tap of the push-pull OT is canceled in the windings, because of how they are wound in the same direction around the core but travel to opposite ends of the total primary winding. So we can tolerate big-ripple at the OT/plate.
But output tube screens amplify from screen-to-plate. Not as much as grid-to-plate, but an amplification factor on the order of 7-12. As a result, hum at the screen is troublesome & louder than hum applied to a primary center-tap.
Single-ended doesn't enjoy the benefits of the push-pull OT, so hum matters at least some at the OT/plate feed. But most amp-designs employing single-ended operation use a small output tube, to deliver lower output-power, which is less current-draw, which is a smaller & cheaper choke.
5v of ripple at the first filter cap might be typical of many amplifiers. The 100Ω/47µF setup knocks that down to 1v, which is essentially a
signal input across the OT primary winding.
The schematic shows 8Ω from White to Black, which will reflect 2500Ω according to the
125ESE data sheet. The impedance ratio is 2500:8, or 312.5:1, and so the voltage ratio is 17.68:1. 1v/17.68 = ~56mV.
56mV across 8Ω is 0.4 milliwatts. Pretty small.
But what if we have a speaker of 100dB SPL sensitivity, like a
Celestion Blue Alnico?
10 log (0.0004w / 1w) +100dB = 10 x -3.4dB +100dB = -34dB +100dB = 66dB.
Hum at the speaker is loud enough to compete with a quiet/moderate TV, but not so bad if the amp is played loud.
Slug the ripple with a 10H choke, and the ripple applied to the OT drops to 18.5mV. OT voltage ratio steps that down to ~1mV into 8Ω, for ~0.14
microwatts. Hum output at the 100dB speaker falls to ~31dB SPL.
The 35dB difference is equivalent to a loudness-difference between a 1w amp and a 3,162w amp.
If anyone goes building themselves a tweed Champ or Princeton clone, they'd be wise in several ways to copy the 5B2-5E2 Princeton, or the 5C1 to 5E1 Champ. Make sure to peep how they set up the power supply in those amps, then marvel at the folks who post on forums about not liking the hum in their new
Fender 57 Custom Champ.