crazydoc said:
I have not been happy with the noise in the preamp at high gain. I bought 100 each of the MPSA18, BC550 and more BC184C's, thinking I could hand select lowest noise transistors for the first preamp stage. I tried 3 or 4 of each, without any notable difference when listening, so I gave up on it. Do you think this or any other mod might be worth pursuing to lower the noise?
You are good! You may have saved me some trouble if you already tried the MPSA18 -- that's my favorite low-noise, high gain transistor and I have used it successfully to seriously improve German mic preamps especially. It is unlikely that more selection from the units you had would give you lower noise.
Microphone preamp noise. . . that's a big subject. If you don't want to read technical, I will summarize that the Neve gain structure and consequently the clone ACMP preamps are not optimized for lowest noise, and there really isn't a lot that can be done about it. In the following tech discussion I will try to be accurate but not mathematical, so forgive me if I simplify a bit to try to give the general idea.
The goal is to amplify a 50 to 200 Ohm microphone with as little added noise as possible. I will use 150 Ohms in the following discussion.
There is an inherent noise generated by any given resistance that is a function of its value and absolute temperature.
Low-noise (like wirewound) resistors generate a noise very close to theoretical. Noisy resistors have "excess noise" which adds to the theoretical.
E.I.N. (Equivalent Input Noise) is usually how mic preamps are specified because of their adjustable gain. It allows one to compare different preamps with different gains by giving a number that represents the equivalent noise at the input of the preamp that will increase by the gain of the preamp.
One must always specify the bandwidth of the noise or one cannot make meaningful comparisons. A preamp that is 3 dB down (signal wise) at 20 kHz might measure better than my 990 Jensen Twin Servo mic preamp which has just under 200 kHz bandwidth. There is way more noise power between 20 kHz and 200 kHz than in the entire 0-20kHz.
to make meaningful audio band noise measurements an accurate brickwall 20 kHz low-pass filter should be used or the measurements are bogus. The 990 will measure way worse, and yet be much quieter to the ear without the 20 kHz filter.
If a preamp has -132 dBu 20 kHz equivalent input noise, then the measured noise level at the output of the preamp is the equivalent input noise + the gain of the preamp. If I have 60 dB of gain I would measure -132 dBu E.I.N.+ 60 dB gain = -72 dBu measured noise at the output of the preamp. In reality one measures it backwards. Measure the noise and subtract the gain to get the E.I.N. By the way, -132 dBu E.I.N. is spectacularly good -- almost theoretical from a 150 Ohm source. When measuring noise in a mic preamp one must always resistively terminate the input with the same impedance as the microphone. I use a 150 Ohm resistor between pin 2 and 3 to measure noise. Shorting the input is cheating and will give an unrealistically low number. Unterminated inputs can give you very audible hiss -- as much as 10 or 20 dB worse noise than a terminated input because the resulting high impedance at the amplifier input is far away from the impedance "sweet spot" that gives the amplifier its lowest NF.
Every amplifier has a Noise Figure (NF). This is how much noise the amplifier adds to the signal it is amplifying compared to the signal's own noise theoretically made bigger with no added noise. The Noise Figure numbers are in the transistor data sheets we discussed a few posts back. For example, let's say that the equivalent input noise of a 150 Ohm microphone is -132dBu. If we amplify the microphone 20 dB with a noiseless theoretical amplifier, the signal from the microphone increases 20 dB and the noise goes up 20 dB as well. No noise is added by the amplifier circuitry, so the signal to noise ratio remains unchanged. However, let's say we use a mic preamp that has noise figure of 3dB (that's really good, by the way). The signal goes up 20 dB but the noise goes up 20 dB+3 dB = 23 dB due to the Noise Figure of the amplifier. The signal to noise ratio got worse by 3 dB in this preamp.
Increasing Noise Figure in mic preamps comes from two main sources, Voltage losses and electronic noise. The DC resistances in the microphone transformer are losses. The signal doesn't go up as much as it would if there were no losses, but the impedance does go up, which makes more noise.
All amplifiers, whether discrete or IC opamps, have a noise figure that is related to the impedance that the amplifier is working with. There are two kinds of noise generated by active circuits. Voltage noise is the noise the circuit makes at very low impedances (shorted input). Current noise is the result of noisy currents being pulled through high value resistances and is the noise that predominates in high impedance circuits. "Low noise" opamps have generally low voltage noise, so they may be very noisy in a high impedance circuit. You would not want to use an AD797 super low noise opamp, for example, to DI interface to a high impedance passive guitar pickup, because it would be horribly noisy.
A 990 or an AD797 or other sub 1 nanovolt/rootHz voltage noise amplifier will have a spectacularly low noise figure when used in low impedance circuits, but have terrible noise when used in high impedance circuits. Every transistor and every amplifier circuit has an impedance "sweet spot" where the transistor or amplifier contributes the least amount of noise (has the lowest NF). The trick to making a low noise mic preamp is to make that 150 Ohm microphone look like the "sweet spot" lowest noise impedance to the amplifer. To do that, one must either design an amplifier with a 150 Ohm "sweet spot", or use a transformer to step up the 50 to 200 Ohm microphone to the higher impedance "sweet spot" of the amplifier at hand.
The low ratio transformer used (1:2) or (1:4 in high gain mode) makes a 150 Ohm microphone look like 600 Ohms or (2400 Ohms) to the preamp input. An optimum amplifier for a 1:2 ratio transformer would need to be very low voltage noise -- like a 990 or AD797 in order to have a decent noise figure. The Neve transistor amplifier will have lowest NF at a much higher impedance. A higher ratio transformer would have been a better noise match to the amplifier, all other things being equal. (They weren't equal, though, because the bandwidth was better on the low ratio transformer so noise was traded away for other sonic benefits).
The heavy loading on the transformer secondary also is bad for noise. For best signal to noise ratio, a microphone should be lightly loaded with a bridging impedance. 150 Ohm mics should be loaded with about 1500 Ohms. This is because we want maximum voltage output from the microphone not maximum power transfer which one obtains from a terminated source. There is a 3 dB noise improvement between terminating a source (150 Ohm source/150 Ohm Load) and bridging the load. Terminating the source drops both the noise and the signal 6dB, unterminated, the signal goes up 6 dB but the noise only increases 3 dB. Rule of thumb, don't terminate microphones if you are trying for lowest noise.
The heavily terminated transformer loads down the microphone so the result is less signal at the secondary of the tranformer than the impedance would dictate if there were no losses. Noise goes up with the impedance which includes resistive losses, but the signal doesn't go up as much, so there is a loss of signal to noise ratio and an increase in NF for the preamp (which includes the transformer). By the way, Jensen transformer data sheets have the Noise Figure of the tranformer included. This is a measure of the the extra noise that results due to resistive losses in the transformer, compared to a theoretical lossless transformer with Zero Ohms resistance in its windings. Because of the resistances in the windings of a real transformr, the output impedance of the transformer goes up faster than the signal compared to a theoretically perfect transformer.
Transformerless designs btw are really bad because the noise generated by the feedback resistor network is part of the noise contribution. That means that for the feedback network to not contribute significant noise, it must be much smaller than 150 Ohms. The amplifier must be capable of driving a sub 150 Ohm feedback network. Real transformerless mic preamps usually only have low equivalent input noise at maximum gain, because that's the only gain setting where the feedback resistor network has low impedance. Their E.I.N. gets really bad at low gains, but in that situation the microphone output is really hot, so it doesn't matter so much.
Because of the transformer's resistive losses, and because we do not want to load down the microphone, it will advantage the noise to make the transformer secondary load as high as possible. The Jensen JT-16-A transformer (which was originally developed as a Neve replacement) is a 1:2 ratio transformer and its optimum load is 6.19K. That's one of the reasons to work on raising the input Z of the first stage amplifier in the ACMP preamps.
Because the first stage has a fixed gain of 30 dB, whatever noise it adds to the signal will be there, and the signal to noise ratio will decline permanently as it goes through the signal path. That's why it's usually a lower noise approach to make the amplifiers variable gain instead of fixed gain. The Neve preamps don't lend themselves to that.
I know that Avedis has done remarkable work in his "Neve" colored preamp. He has reworked the gain structure significantly to fix both the microphone loading problem, the transformer loading problem, and the noise problem.
None of the clones do that. They just copied what Neve did, both the good and the bad.
Well this post is already ridiculously long. Hope it is helpful to clarify why designing really good audio gear is more complicated than it may first appear.