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could somebody explain me how does this audio amplifier circuit from old radio is working ? I understand role of last transistors 413,417 and 415,419 but what is the point of T409 and T411 and other blocks ? Another question is why we feed input through differential amplifier ? Btw do you guys know any good resources about old audio equipment design ?

amplifier schematic

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  • \$\begingroup\$ The diff amp handles the feedback. I assume T409 and T411 temperature-stabilize the 0-signal current through the end transistors. \$\endgroup\$ – Wouter van Ooijen May 16 '16 at 20:47
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    \$\begingroup\$ T409/411 are current limiters. When the voltage across the emitter resistors at the output stage is enough to turn on T409 or T411 they start conducting and steal current from the bases of T413/415 respectively, causing clipping (rather than thermal runaway). \$\endgroup\$ – user207421 May 16 '16 at 20:54
  • \$\begingroup\$ Ok , thanks for that explanation and do you have an idea why resistor in the lower middle (R418) is variable ? why not typical resistor but poteniometer ? \$\endgroup\$ – molok May 17 '16 at 1:05
  • \$\begingroup\$ @molok The reason for R418 is in my answer. \$\endgroup\$ – user105652 May 17 '16 at 1:17
  • \$\begingroup\$ That looks very much like the Leech Amp (users.ece.gatech.edu/mleach/lowtim). If you are interested, his web page has everything about how to design a quality audio amplifier. \$\endgroup\$ – b degnan May 17 '16 at 1:31
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It may be an old design, but it is still in use today, especially in car stereo amplifiers. What has changed is the quality and performance of the transistors. You asked a few questions, so I will just go stage-by-stage.

1) The differential input is much like that of op-amps. It allows for some gain and a balanced wide-band response and DC stability.

2) T401 is the signal input while T403 is the feedback from the output. This sets the gain of the amplifier to about 10 or less. It stabilizes the amplifier so with no signal in there is zero volts at the output. T401 feeds the signal to T407, which is a level shifter and adds some gain as well. T407 drive the output stage, through T405 which sets the bias(idle) current for the output transistors.

3) The more bias the less distortion, but the hotter T417 and T419 become. R418 (bias current adj)has to be trimmed with great care so the distortion is low but the outputs will not overheat. C410 creates a 'boot-strap' current fed back from the outputs that boost the drive current to the output stage, by just a small amount, increasing the maximum volume that can be put out to the speakers.

4) T13 and T417 form a NPN darlington and T415 and 419 at as a PNP darlington to act as a buffer for the signal at the collector of T407, which is already at the maximum voltage swing possible (at full volume). These darlington's allow the output to drive a low impedance load such as a speaker.

5) T409 and T411 protect the output stage from excessive currents by clamping the drive signal. This can cause distortion at high volume, but it is a warning sign that the volume needs to be turned down until the distortion stops.

6) R440 and C424 act as a small load at certain frequencies where the amplifier is unstable, and keep the amplifier from oscillating at those frequencies, regardless of the speaker load.

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  • \$\begingroup\$ very nice explanation , thanks for that , if you are curious it comes from that polish radio : oldradio.pl/karta.php?numer=913 \$\endgroup\$ – molok May 17 '16 at 9:02

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