ricardo said:
With the 'high' voltage BC560s, D2 & 3 don't have to be Zeners. They could be 1n4148 or any number of SMD double diodes. But you must have them or else a momentary cable short will zap the base emitter junctions. The mike will still work but be forever noisy.
I had just copied the 6v2 protection diodes as fitted in the original Schoeps CMC5 schematic ... I see your point of them simply acting as diodes, should either pins 2 or 3 be shorted directly to ground - but I had always assumed that using a zener was to protect against excess voltage presented across the transistor, in the event of the 47uF cap being fully discharged.
If it was then presented with a 'live' phantom power 'plug in' it might present excess voltage across the CE junctions before the capacitor was charged?......
A bit remote I would have thought? .... but as Schoeps had fitted them - and at a cost of only at 3p per diode - I decided 'hang the expense'!
ricardo said:
If my understanding of the noise sources is right, damping T2 secondary will reduce noise & signal equally for no difference in S/N
Yes of course..... I had assumed that the dominant noise source might be the resistor noise from the source and drain resistors, which is 'post' attenuator... but a quick practical test confirms your assumption that the noise floor is indeed reduced as well.
(I do need to confirm the actual values for the -10 and -20 dB pads ... the provisional values of 3k3 and 1k on both the AMX9 and AMX10 schematics may not be correct...
ricardo said:
My musings about feeding the rectifier directly from the bridge come under 'stuff that must be tested' but, IF they work they MAY improve & simplify stuff.
I looked again at Baxandall's paper and found this comment on page 594:
"....Ordinary conversational speech at a foot or two corresponds to about 1 dyne/cm' alternating pressure, and this causes, with a typical modern electrostatic microphone element, a capacitance change in the region of 0.001 pF....."
I decided that's not a lot! - and changes that small would need all the help they could get.......
Hence my decision - at this stage - to stick with the 'noise free' gain from the step up voltage - and 'Q' - provided by T2 ....
Khron said:
Isn't the oscillator power already sort of "isolated" by R2 and C6? I suppose one could "guild the lily" and replace R2 with an inductor, for extra HF / RF filtering...
...
C6 was fitted to decouple the collector of the oscillator transistor, which helps with the linearity of the oscillator waveform ...R2 was selected to allow the optimum oscillator level - at max 'Q' setting - to be determined.
The idea of C14 was to add extra decoupling to keep any HF zener noise out, should the electrolytic not be good enough at high frequencies.
In fact it would also act - with R2 - as a low pass filter to help keep any remaining oscillator noise away from the drain resistor as well.
In the past, I have had problems with HF noise and electrolytics, - but that was some years ago, and modern electrolytics are probably much better with HF..... old habits die hard!