Q7 and Q10 are always on Mark.
Q10 derives its collector and emitter current from the B+ rail through R23 as a static voltage source.
R34 is the primary equivalent of R23 for Q7's emitter and collector current which basically scavenges this current off of the bias current produced by the upper half of the amp, Q11 and R38 at idle and off the emitter currents of Q13-Q17 when the amp is actively driving the upper half of the signal. The source for Q7's emitter and collector current is thus dynamic, not static and thus unlike the upper half.
If the global feedback demands of the amp are such that Q5 is calling for more "down" signal and Q7 cannot provide that through R34 alone, the voltage drop produced by the current flowing through R34 will eventually turn on D13 and provide "turbo boost" allowing more current to flow through R35 as well. In the case of large reactive loads on the output this is often important in order to "tame" that load.
This is the readers digest summary of how this works.
The local feedback works a little different. In the presence of current drive from Q7 which is a classic emitter follower connected to the output signal of the amp, current amplification of Q7s current is provided by Q12, Q14, 16, etc. UP TO THE POINT that Q12, Q14, 16 etc. saturate to the point that they begin to cut off the emitter of Q7. When that point is reached, the current drive provided by the collector of Q7 to Q12, Q14, 16 etc. dries up and an equilibrium is reached and it drives no farther than demanded by the emitter node of Q7. This is the local feedback path I am referring to. The self regulating loop formed by Q7, Q12, Q14, etc.
There is significant voltage as well as current gain provided by Q12, Q14, 16 etc which can lead to instability in this local loop. This is unlike the upper half which is a straight emitter follower triad (Darlington) configuration with NO local feedback.
Tricky to describe, I hope I did it some justice.
Q10 derives its collector and emitter current from the B+ rail through R23 as a static voltage source.
R34 is the primary equivalent of R23 for Q7's emitter and collector current which basically scavenges this current off of the bias current produced by the upper half of the amp, Q11 and R38 at idle and off the emitter currents of Q13-Q17 when the amp is actively driving the upper half of the signal. The source for Q7's emitter and collector current is thus dynamic, not static and thus unlike the upper half.
If the global feedback demands of the amp are such that Q5 is calling for more "down" signal and Q7 cannot provide that through R34 alone, the voltage drop produced by the current flowing through R34 will eventually turn on D13 and provide "turbo boost" allowing more current to flow through R35 as well. In the case of large reactive loads on the output this is often important in order to "tame" that load.
This is the readers digest summary of how this works.
The local feedback works a little different. In the presence of current drive from Q7 which is a classic emitter follower connected to the output signal of the amp, current amplification of Q7s current is provided by Q12, Q14, 16, etc. UP TO THE POINT that Q12, Q14, 16 etc. saturate to the point that they begin to cut off the emitter of Q7. When that point is reached, the current drive provided by the collector of Q7 to Q12, Q14, 16 etc. dries up and an equilibrium is reached and it drives no farther than demanded by the emitter node of Q7. This is the local feedback path I am referring to. The self regulating loop formed by Q7, Q12, Q14, etc.
There is significant voltage as well as current gain provided by Q12, Q14, 16 etc which can lead to instability in this local loop. This is unlike the upper half which is a straight emitter follower triad (Darlington) configuration with NO local feedback.
Tricky to describe, I hope I did it some justice.