by PRR » Tue Dec 28, 2004 10:38 pm
Not to do Tim's work, but just to gauge what level of explanation you-all want....
> Why a 1:10 transformer is appropriate for a 2520 but not for a 990 opamp which wants a 1:2 and how these three subjects interact for optimal design.
It isn't ratio but impedance. The numbers you give are customary because most mikes are about 150Ω. If we liked 10Ω or 2,000Ω microphones, we would use different ratios.
(However, a very long length of twisted shielded cable works best at about 100Ω-300Ω, even with large changes in cable dimensions. And there are situations where mikes are very far from their amplifiers. So the 150Ω impedance range is pretty well forced upon us.)
Remembering (from a prior yet unwritten chapter) that impedance scales as square of transformer ratio: with 1:10 the amplifier sees 150Ω*10*10 or 15,000Ω; with 1:2 the amplifier sees 150Ω*2*2 or 600Ω.
The noise of a transistor (or anything) can be considered in two parts: a noise voltage and a noise current. The noise voltage adds to the signal voltage. The noise current flows through the source impedance and creates a voltage that adds to the signal voltage.
Hmmm.... we have a voltage and a current, sounds like a resistance. In fact you can see it that way too.
As you increase the transistor current, noise current increases (logically) and noise voltage decreases (for reasons we can defer to another chapter). So the noise resistance of a transistor varies with the bias current.
The 2520 uses a fairly low bias current, perhaps around 0.1mA. The 990 uses a fairly high bias current, I think around 2mA. The optimum source impedance for the 2520 is much higher than the optimum source impedance for a 990.
But wait, there's more. Before transistors there were vacuum tubes, which have negligible noise current. In classic low-noise tube design, you use the highest possible step-up. (For reasons covered in the transformer chapter) 10K or 20K is about as high as you can go for good wide-range audio response. So when transistor amps appeared, the world was full of good 1:10 transformers, and that's what designers aimed for. System impedances tended to be around 10K.
But many designers started exploring the high current possible with transistors. Working at low impedances and quite high current and power, a transistor can equal or exceed the signal to noise performance of a tube. Deane Jensen's 990 (among others) targetted very low source and feedback and mixing resistors. System impedances tended to 600Ω or less.
And as in life, a happy medium is better than going to extremes. Both the 2520 and the 990 approaches can work fabulously well, but so can 2K-3K impedances.
> how you use IV curves to set bias and then still be able to control the gain of the transistor stages.
The gain of a transistor amp is NOT set by bias current. Well, it has an effect.... you can show this by setting up a 1-transistor amp with a fixed load resistor and an adjustable current. Gain is proportional to current. BUT the input overload point is only 10mV-20mV, and the distortion near that point is about 26%! You can't make hi-fi amps that way. Moreover, in a real amp the bias current will change from part to part, and with temperature, so the gain is never the same unit-to-unit or day-to-day. BJT transistors always use feedback to set the gain.