Horse, I see no big deals, at least from me. I was just trying to have a conversation (evidently one-sided

) about what I find to be an interesting technical aspect of tube operation. I grant it is waay off topic, but that seems to be the norm around here after a dozen or so pages.
That said, I have never seen burned grid stopper resistors. But I have seen amplifiers oscillate without them and will not rebuild a Leslie amplifier without them being added. Some tubes ain't what they used to be.
Thanks for the graph - provides a missing link and tells its own story
As for "
waay off topic", the thread is SS Class D v Tube Amps. Tube guitar/bass amps mostly operate in Class AB so the comparison must inevitably be between Class D SS and Class AB tube
The discussion was about deliberate overload distortion in the power stage and how that might be achieved in a Class D amp - compared with using dummy load devices with tube amps. Aged Horse quoted a figure of 10% at rated max power so we are talking about the range of progressive distortion between and 10%
DavesnothereCA said:
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OK, it could have been some other factor which the lead players like about the way in which tube amps broke up when pushed, but that was what anecdotally reached me at the time.
And as I am sure that you recall, companies came out with dummy load boxes (such as from Altair and Tom Scholz), to let a player variably dial down the final volume to the speaker while pushing a power stage just the right amount, whatever THAT was. ~
Seems everyone is forgetting that the "B" in "AB" means Class B
In my understanding that the transition into Class B operation has the effect that grid current will flow during that part of the cycle when the grid is driven positive - i.e. above zero
That current, which is audio signal current - must be supplied from somewhere - normally the driver stage
So to clarify - In a fixed bias system at zero signal the grid bias is determined by the DC bias supply. MI tube amps typically include a DC bias adjustment mechanism to one or both power tubes to optimise performance and limit the current flowing through the tubes to a safe level within dissipation limits. At zero signal audio power output to the speaker would normally be zero (residual hum and noise excepted).
To cause a change in plate current and therefore power output it is necessary to change the grid bias positively or negatively as applicable in response to the signal amplitude. That task is performed by the driver stage immediately preceding the power tubes
The advantage of transformer drive is that phase splitting is automatic, accurate, reliable and can be driven by a single power tube (the transformer does the phase inversion)
The advantage of RC coupling is that it saves cost and weight but introduces significant resistances into the grid bias supply circuit. It is also challenging to achieve exactly equal signal drives to each tube. Many of the vintage tube amps use half-wave rectifiers, further reducing the capability of the power supply to maintain a stable DC bias under grid current conditions. Application of negative feedback from the speaker further complicates the system as it tries to self-correct.
Taking into account the "duty cycle", which thanks to various contributors we now know is about 12.5 % for a bass amp, we can say that Class B operation will only typically occur in the asymmetrical peak of the first half-cycle in a normal note - and when it does it will only be for an extremely brief time period
So while the 6L6 curves show substantial grid current for all positive grid voltages, in practice it will not be for long. The average plate current over the full cycle and subsequent cycles will be significantly less and it must therefore be assumed that this is the reason Class AB bass amps are not self-destructing on a massive scale
But the graph also shows that if a 6L6 amp is overdriven continuously - such as with sustained echo - then the ball game changes
Also if the duty cycle equivalent is sufficiently compressed it will no longer be 12.5% but something greater. If the dynamic transient peak at the start of the waveform is removed by compression then the average wave must be of greater area under the curve - ie have a higher average power value
The conclusion then is that if a bass amp is played within its design limits it will do a great job reliably but if pushed too far anything can happen along the path to self-destruction
The discussion on grid resistors has drifted into a distraction from the main thread. When one is faced with an amp which has shorted power tubes, shorted output transformer, shorted power transformer and fused grid stoppers then one can only speculate as to a first cause. I tried to present an explanation for one possibility.
For me, seeing is believing, so if you have not experienced these events then it is difficult to convince you. The doubters are also prepared to abandon proven textbook theory as to how tubes work.
Despite many posters suggesting tube amps are a historical novelty, there are still many bass players out there who are not only using them but prefer to buy them new instead of cheaper SS alternatives. To each his own.
They are the folks I have been talking to.