Mr. Marsh's neat MC preamplifier

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RNM published this design in The Audio Amateur 1/1982 -- there were a couple corrections in 2/1982. It features very low input impedance and use of easily attainable components, no "impossible to source high gm P-jfets". I've changed the schematic to reflect the corrections, and updated to include the OnSemi devices which are readily available as well, and more easily attached to a heat sink:

An externally hosted image should be here but it was not working when we last tested it.


It was suggested in the "Bipolar Transistor Tester" thread that 2N4400/03 would be lower noise. Of course component values would have to change. Could also use the THATCorp low noise P and N matched transistors.
 
The 2N5210 and 2N5087 aren't ideal because they have a base spreading resistance of around 150 Ohms, if I recall correctly. Quad used the Zetex ztx650 and 750 in their MC preamplifier in the QUAD 44 and 34 because of the very low base spreading resistance of these transistors. Toshiba made transistors with incredible low base spreading resistance that would be ideal for this application but they seem to be unobtainable now.
 
You can make a good estimate of the Rbb by looking at the graph of voltage noise (nv rt Hz) vs collector current. Typically the noise decreases with collector current and bottoms out at some low value. Calculate the resistor value that gives that noise. Just remember, 1K resistor = 4 nv rt hz, 250 Ohm = 2 nv rt hz and 62 Ohms = 1 nv rt hz.
 
Got me to think of how to measure Rbb directly -- Burkhard Vogel has a method in Chapter 5 of "The Sound of Silence" --

Just fit the input noise vs Ic to a plot of the root-sum squared re and rbb. The rbb that makes the best fit is a good guess. There are high current effects that can mess things up a little at large Ic so you might not get a perfect relationship but good enough.

There is a web site that uses RF power transistors that are even better (at least the npn) than the Toshiba devices were.
 
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You can make a good estimate of the Rbb by looking at the graph of voltage noise (nv rt Hz) vs collector current. Typically the noise decreases with collector current and bottoms out at some low value. Calculate the resistor value that gives that noise. Just remember, 1K resistor = 4 nv rt hz, 250 Ohm = 2 nv rt hz and 62 Ohms = 1 nv rt hz.

Here's the MPSA18 datasheet http://www.onsemi.com/pub_link/Collateral/MPSA18-D.PDF

I guess you're talking about Figure 2. Looks like noise bottoms out at 3.6 nv rt hz which is equivalent to an 810 ohm resistor; is that your estimate of Rbb?
 

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The figure you posted shows the noise voltage increasing with current rather than decreasing.
Oops, yes you're right! I posted Figure 2 of the MPSA18 datashseet, but Figure 3 might be closer to what member rayfutrell had in mind. Interestingly the "bottom out" point is about the same, approx 3.6 nv rt hz, leading to the same estimate of Rbb, 810 ohms. But 810 ohms seems awfully high.
 

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I have a cartridge with 4 Ohm impedance so yes, i say 10mA makes a difference.
It may not be big but even in your graph you can see the difference at lower impedances.
Is that 1 or 2dB ?
Also when you make an open loop phono stage the higher Gm on higher idle can be an advantage.

If you optimize Noise with respect to I(collector) -- this visual should demonstrate how much there is (or is not) gained:

An externally hosted image should be here but it was not working when we last tested it.
 
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