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Low distortion audio amplifier
Low distortion audio amplifier
 This is an unusual circuit for an ultra-low distortion power amp.  According to my original notes the circuit is dated January 1977 so the  circuit is not exactly modern but it is still sufficiently different to  be interesting. The circuit was designed and sold as a card by a  purveyor of surplus components but, even using mostly manufacturers  rejected transistors, we managed to get about 0.02% total harmonic  distortion at 30 watts with a ±25v power supply into 8 ohms.: no bad  figure even in these days of MOSFET and ICs. In 1977 anything below 0.1%  was considered excellent. And this figure was pretty repeatable without  doing much selection.  
The problem of course is that since I havent touched this amplifier for many a year I have absolutely no idea what modern transistor types one should use for it but they are not critical: output transistors and drivers need to be the correct type but the other transistors can be small signal types - as long as they can handle the full voltage between + and - supplies.

The problem of course is that since I havent touched this amplifier for many a year I have absolutely no idea what modern transistor types one should use for it but they are not critical: output transistors and drivers need to be the correct type but the other transistors can be small signal types - as long as they can handle the full voltage between + and - supplies.
Tr1 and Tr2 are a long-tailed pair (LTP to save typing). It is quite  common to have a LTP in an audio amp but this is different: this is a  complimentary LTP. As far as I am aware no one else had used a  complimentary LTP at the time, though I have since seen it used in one  other circuit. So I guess the circuit is unique to the author. One of  the things that limits the performance of a conventional LTP is that the  tail source loads the common emitters. In a complementary LTP this  cant happen as there is no tail current source so that all the current  of one transistor has to flow through the other. 
Tr2s collector current flows into D1 and D2 which develop a  voltage: this is used to bias Tr8 as a constant current source for Tr4s  collector. The fact that Tr4 is working at a constant current defines  its base-emitter voltage which must be developed across R4. This defines  a current in R4 and this is the current that the LTP must operate at -  so the ring of four transistors (Tr1, 2, 3, & 4) is self biasing and  all transistors work at their best with minimum unwanted loads and  biasing detracting from the performance. Tr4 is actually one of the most  critical transistors: in the original circuit it was selected for Vce  greater than 75v. Most Texas BC212s passed easily. Lower voltage  transistors caused an increase in distortion level. 
There is always a down side to any circuit: in the conventional  LTP the base-emitter voltages tend to cancel each other out. In the  complimentary LTP they add so there is a drop of about 1.2v between the  two bases: this must be cancelled in the biasing chain and, since this  circuit was designed for operation over a wide range of supply voltage, I  had to be a little clever. Because of the constant current operation of  the LTP and the constant voltage drop across D1 & D2, there is also  a constant voltage across R14. This drop is used to lift up the bottom  of the biasing chain (R1 and R11) so that the output sits at around half  supply voltage, over a wider supply range. 
D3 and D4 develop a bias voltage so that the output transistors  are at the correct point, slightly conducting, to minimise crossover  distortion. 
The output transistors are complimentary (the original design  used MJE2011 and MJE2021) and are driven by complimentary drivers: PNP  driving NPN and vice versa. This arrangement is not only pleasingly  symmetrical but gives better performance that the more common Darlington  arrangement - the full gain of all the transistors is used and there is  more internal feedback and less voltage drop. 
The output current is monitored in the two resistors R7 and R22  (180 milliohms). The current limiting is unusual in that it works inside  the input ring at an earlier stage than normal. This has an advantage  that the current limiting transistors do not load the drive circuitry -  which will introduce distortion. The slight down side is that there may  be a slight tendency to oscillation when in current limit. R3 and R14  are necessary to restrict the current availability when the current  limit engages. R5 and R19 are present to make the current limit vary  with the voltage across the power transistors to avoid the second  breakdown region of power transistors. 
The points shown connecting terminals 1-2 and 6-7 are  scratch-through tracks. 1 and 2 are the power and signal earths: to  keep distortion in a stereo system to a minimum the currents in these  must never share the same path so in a stereo system four earth wires  are run to the systems common earth point - a spider common earth -  and this means breaking the link. The link between 6 & 7 is in the  feedback path and there are times when this can usefully be broken - one  cheapskate was to fit a tone control circuit here (see below). It  works fine but is a bit of an insult to such a low-distortion design!. A  third break point is in the collector of Tr2. Breaking this shuts down  the amplifier completely and safely. Is a thermal switch is to be  fitted, this is the place. 
Overall negative feedback is in two parts: D.c. is fed back via  R13: there is 100% d.c. feedback. A.c. feedback is via R12 and R17. Note  the output capacitor is inside this feedback loop (speaker connects  between terminal 5 and negative) which extends the low frequency  response. 
Another feature is the accessibility of both ends of the output  coupling capacitor: being designed for a junk shop, they didnt want to  use expensive capacitors! So for extra bass performance an additional  capacitor can easily be connected. 
The circuit can also be driven as a low input impedance: break  6-7, short pin 8 to C4s positive and apply input to pin 6. In this mode  the input distortion is actually better: my original notes show as low  as 0.01%!  
When building a low-distortion amplifier, layout is vital. In  fact to get distortion around 0.02% requires a lot of skill and  experience. The problem is that the current in the output stage  alternates between the two power transistors so is a rectified version  of the input. Now there is no such thing as a wire. Any real piece of  wire or copper track is a resistor with associated inductance and  capacitance. If the high current, rectified output signal mixes in the  same piece of wire with the input signal the distortion in the  rectified output current will feed into the input and cause the overall  distortion to rocket. This is something which cannot properly be taught  but has to be experienced. A skilled audio engineer will spend his  lifetime learning about it. 
Source by : http://www.4qdtec.com/pwramp.html 
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amplifier,
audio,
distortion,
low
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