"Alte Schule" - The five-minute amplifier approach!

I understand your thermal objections, they are not to be dismissed out of hand - and probably only a test setup will shed more light here, I am thinking of the actual disaster - of the extent.

There is no question that there is a worm in the apple here. First of all, I insert the bootstrap.

1733821045782.png


THD is now -86dB

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My /our original idea was (and is) to transform the present model in such a way that a functional and at the same time magical current dumper circuit is created. For what other reason should RF be so low impedance and be exactly 500 ohms?

However, I need the active support of all Currentdumpers for this magic - cooperation is again kindly requested. I have already wound a 4µ7H air-core coil.

🤔
 
(...) solder and test a "5 minutes" amp (...)
I think about that all the time, constantly - but the ravages of time are gnawing away at my limbs.

And above all, I own a flawless REVOX A78
(whose power amplifier module is already pretty close to the five-minute approach).

Young people are welcome to pick up a soldering iron, they have my support ..!

😎
 
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@astx

Before I get started, I have to get the 3/4 + 3/4 amp up and running with @m0rten - heck, I have a new amp idea every few minutes, with the RIAA equalizers it's even worse, by the second. And @stv is also in the starting blocks with the Beelzebabe amp, and the construction sites are piling up. The AA50W also wants to be looked after and the 25-Wwatt Krill is also waiting impatiently.

And my wife really wants to visit Vienna with me.

So for the time being, we're staying in the first development phase of the five-minute amp, and it's all modern, purely digital and virtual with MC12.


Grüße,
HBt.
(PS erwähnte ich bereits, dass ich beim Thema Lautsprecher nicht ganz unbelastet bin?)
 
It should be noted that the present design also has two inputs like the usual blameless variant. The base of Q5 is our positive input, its negative input follows the positive input - but now the negative input (Q5's emitter electrode) also represents a node, a summation node for currents. With its size, RF now essentially determines the resulting bandwidth of the now negative feedback system; RN is almost single-handedly responsible for the gain.

A special feature that should not be underestimated.
 
I don't see what purpose R1 has. If you want to measure the voltage across a resistor to measure the quiescent current, you can measure across R2. If the emitter of Q2 were connected to its other side, it could improve thermal stability by limiting the transconductance at large current levels, but that is not applicable.
Normally, R2 is very rarely located at this point; on the contrary, it tends to slide upwards, i.e. between the collector of Q7 and the output node. While the emitter of Q2 is now also located on /at the output node.

And so on, we all know this - and simply don't dare to play a little more and explore other points of view. Especially if they still seem nebulous.


I simply have the same concern as Ed. Suppose you play loud signals for some time, causing substantial power dissipation in Q6.
I have understood that and it is a really good point, which goes even further, namely to the question of whether various protective devices are still missing for safe operation. And they are still missing completely, but they are not an issue at the moment. This litter /throw should not be able to deliver much more than 16 real watts.


Due to the thermal resistance from junction to heatsink, Q6 will then become hotter than Q1, Q2 and Q4. As a result, its Is increases, or in other words, its collector current at a given base-emitter voltage increases.
Oh, I see the EbersMoll number.

We also have the option of modifying the Vbe multiplier.

If Q6, Q1, Q2 and Q4 are mounted on the same heatsink, the temperature-dependence of Q6 is only partly compensated for by Q4 due to the temperature drop across the thermal resistance from junction to heatsink of Q6, that is, due to Q6 being hotter than the rest.
I have no plans to thermally couple Q1 & Q2 with Q6.


If this causes thermal runaway, the amplifier will self-destruct.
Of course, this must not happen and must be prevented, how?

If the self-heating due to the increase of the quiescent current after playing loud is much smaller than the self-heating that caused it, it is not a big problem, although it still worsens the dependence of the distortion on the programme dynamics.
So here I have a knot in my brain; let's leave out the self-heating and consider everything else as external heating (including that caused by the required dynamic load current).
What does the situation look like then, and what influence does this part really have on the instantaneous THD?

Our fears relate solely to Q6, which in itself is absolutely nothing more than an emitter follower (with all its consequences and positive characteristics) - for Q7 it represents a dynamic load (or current source).

With this view, however, R2 suddenly comes back into the picture - the old masters at Studer /Revox even set R2 to a value of 1 ohm ..!

It might have its advantages to put Q1, Q2 or both on a separate heatsink.
In the given topology, there are some interesting thematic coupling variants, I keep saying that.
Q1 & Q2 are usually located together on an extra heat sink.

Due to the gain of the VBE multiplier, the self-heating of Q6 may then even be overcompensated. I don't really know what effect the thermal capacitance of the main heatsink will have, though.
Either you try out the whole scenario in practice and experiment a bit (aids are: cold spray, the soldering iron, a hair dryer ...), or you set up a model and simulate the whole thermal snot.


#
As I've already written, I'm not actually that extremely worried - but the scenario we've outlined is still very frightening.

What should we do now?
There must be a solution - if the solution is the problem [loosely based on Paul Watzlawick].
 
Last edited:
@wahab
I had actually hoped that we would use the circuit shown here as a basis for a conversion to a "current dumper". The aim of this surgical intervention must of course be to allow the already quite low THD of (min)0.001% to sink to unimaginable depths, at least to 0.00001% flat and horizontal for the entire frequency and power range.


😊
 
So before I tinker with a voltage regulator IC as an audio amplifier, I'll just use the good old LM12. If everything is well prepared, I only need ten minutes with the LM12.

FYI
look into the attached pdf

LM12 is well known, that was an exceptional opamp, guess that the LM3875/3886 are derived fom this chip,
although nothing is as rugged as the TO3 ancestor.

My point was that with a too low xtor count 2 stages amp perfs wont be worth the effort, with this kind of design
the good balance is 7 transistors excluding the VBEM, otherwise that s a waste of ressources, i ll post some schematics
to clear this point.
 
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