> use two diodes as the Vbe reference and divide it down to one Vbe plus a smidgen. ....It just burns my biscuits to see 18 mA or so being burned off...
I wuz wondering where all that current was going.
One "righter way" is to grab a third output device and a couple of resistors, a Vbe multiplier. The 3rd device WILL be the same Vbe as the outputs, +/- temperature and currrent. Unlike most diodes, it has a hole to nail it to the heatsink. I forget what your output current is, but if you want 60mA there and 1mA in the reference, at 60mV/decade, then you want almost 120 more mV on top of the 1mA Vbe. Take the base-emitter resistor much larger than 600mV/1mA or perhaps 5K. Put a 1K trimmer collector-base. You can get from 1.0 to 1.2 times the 1mA Vbe, which should bring the output devices to good heat without huge heat in the reference source.
Or you could stack three #47 lamps down from your +18V to a diode and get a large Vbe reference plus enuff light to read by.
> I'm not exactly sure why it takes 44! op amps either to make a stereo HP driver
I've used 8, plus a quad of 3055/2955 power devices. Pure Class A to 250mW and heavy NFB.
Figure a 5534 will pull 600 ohms well. 600/32= 18.75 chips, 37.5 for stereo, which rounds-up to 44 easy. (They may like me have a complex gain-control structure before a fix-gain power array; or balanced inputs or other frills.)
> something to the stiff high current voltage-source drive on the 1646 output that works to our advantage
There's a simple "proof" that a good BJT near-B stage should drop 28mV in emitter resistors to get first-order compensation for crossover distortion. Going low is nasty and going high brings up 3rd but reduces 5th, 7th, etc. Indeed stage-amps are often biased 20mV (cool is good) and hi-fi at 30mV-50mV.
(And THD numbers this way are lower than in Class A. The two devices are not fighting each other and driving-up the THD.)
That 30mV-50mV in Re is correct only if the drive impedance is ZERO.
For non-zero Z drive, I believe you divide source Z by Hfe and subtract that much from Re.
If you could have true hi-Z drive, Re seems to be zero. Indeed true current-drive would not invoke voltage-threshold crossover distortion. But what current driver has infinite slew?
But most such amps (and IIRC that 990 you were making fun of) take capacitive NFB from the drive point. In the top of the audio band, the source Z to the output devices may fall quite small. Since abusive overall NFB will kill bass crossover, you pick idle current and Re for the high end of the band, which is where drive impedance is typically low.
> I used a NPN and PNP common collector, .., I tied both bases together and to the opamp output, then used a resistor divider from the two emitters
A similar ploy was once popular as a video line driver. Aside from lo-Z base drive, I guess it was Class A (AB cutoff recovery time is a problem at 5MHz on 1970s parts), short-proof, had benign clipping, and a defined output impedance through the resistor string. This was +12V power and coupling caps, so DC offset was not an issue. The gross waste of power was orders of magnitude less than the tube amps of a generation before.
> 4V P-P driving some old Koss PRO-1As.
???? 10mW? You the guy who likes "big loud manly headphones driven really loud"????
You musta missed Hot Tuna in their over-loud days. 10mW is kiddie-level.
OK, I do work near 1mW-2mW most of the time, but my 100mW amp wasn't enough for live recording monitoing, why I built the 250mW. I can't clip it with Pro-4 phones and live, but some modern phones (the kind that don't sound like wider-range telephone earpieces) will clip 250mW before my eyeballs bulge. (Kids, don't try this at home. You'll end up like some of our recent students: obviously half-deafened by iPod addiction. And these are musicians!)