Paul, thanks for all the work on 'rectifier' transformers.
I'm no expert on any of this stuff, transformers are not my game, but in summary here are the requirements for a SS Class AB power amplifier:
1. Low EM emissions for elimination of induced hum in the signal path.
[Favors toroidals at low idling currents where hum is an issue.]
2. Low magnetostiction for reduced mechanical hum.
[Favors EIs and C Cores which stress their cores less and are more robustly made and varnished, thus leading to less mechanical force moving the laminations.]
3. Low weight for reduced shipping and mounting costs/difficulties.
[Favors toroidals.]
4. Low magnetic flux density at full rated power so as to avoid core saturation and flattening of the AC waveform, which leads to high order harmonics difficult to filter out.
[Favors EIs and C Cores since most toroids are build with flux densities within 20% of the 1.6T flux limit of standard magnetic iron.]
5. High magnetic flux overload capacity so that large current pulses during cap charging do not distort the waveform.
[Favors large dimension iron such as EIs and C Cores.]
6. Relatively low self-inductance in secondary windings so that current pulses during cap charging do not suffer voltage drop.
[Favors toroids which run shy on copper.]
7. Tolerance of DC on the mains.
[Favors EIs and C Cores which have large magnetic circuits.]
8. Low emissions of current pulses back into the mains.
[This favors toroids, since they are limited in current pulse delivery. This is very important since reverse emissions are becoming crucial, with the EU in particular mandating low noise injection back into the mains for future transformer designs. This is actually driving SMPS, regrettably.]
As you can see, the benefits are distributed. However, my experience has been that the best compromise is an EI designed for conventional M4 laminations but running Grain Oriented Silicon Steel (GOSS), which has almost double the magnetic flux capacity, around 2.8T.
You generally find that 'rectifier' transformers (so named because they are designed to drive full wave rectifiers with large capacitive smoothing, just like an audio amplifier) are EIs, built to generous dimensions.
Using the above philosophy, I specified GOSS EIs for the GK1, and these have been extremely successful. They are dimensioned for standard M4 iron, but built with GOSS laminations. EM emissions are very low, current pulse delivery is very high, and even constant current delivery is almost four times nominal rating. Size is small, and mounting is easier than a toroidal.
There may well be errors in some of this, since it's all top of the head stuff in the limited time I have available to me. I don't like making categorical statements because someone always shows me up, but I think this is pretty accurate. Any corrections, please, let's have 'em.
A very good idea I discussed just yesterday with Andy Redwood in a pleasant cafe here in Heidelberg was constructing a 300VA toroid on a 1000VA core. This would be physically very much larger than the normal 300VA toroid, but most of the advantages and none of the disadvantages of toroids would be available to the designer. However, I'd rather deal with EIs, largely because they are the sort my supplier specializes in and knows so well.
I should mention that Matt has not done his definitive transformer test between toroids and Double C cores, so unfortunately I can't give any comments just yet.....
Cheers,
Hugh