Cello One. Good Amplifier 15 Watt with TMC and Laterals

I agree with bonsai. C7 is a double-edged sword.
C7 is for canceling the input capacitance of U2 and must be selected so that C7/(input capacitance) = R8/R9.
If it is too large, ULGF will be postponed and it will become unstable.
Usually, it has a small capacitance of about 1p to 3pF.
I think it would be better to lower the impedance of R8, R9, and C1 further (e.g. 470Ω, 6.8kΩ, 220uF) to drive the extra pole formed by the input capacitance of U2 to higher frequencies.
This would mean changing resistor in the input as well. 6.8K is very low input impedance.
 
I agree with bonsai. C7 is a double-edged sword.
C7 is for canceling the input capacitance of U2 and must be selected so that C7/(input capacitance) = R8/R9.
If it is too large, ULGF will be postponed and it will become unstable.
Usually, it has a small capacitance of about 1p to 3pF.
I think it would be better to lower the impedance of R8, R9, and C1 further (e.g. 470Ω, 6.8kΩ, 220uF) to drive the extra pole formed by the input capacitance of U2 to higher frequencies.
I might try lower the value of C7.
1pF to 3pF.
But as it is now it works okay.
It was @minek123 that added the C7 for me.
 
I would seriously recommend that the TLV431 be replaced with a red LED. They have a forward voltage drop of 1.8V and about the same dVbe vs temp as a transistor ie -2mV/K. This will at least give the current source 1st order cancellation of output current dependency upon temperature which it does not have now (it's about 50uA/K right now, so over a 30-degree temp change, expect the current source output to shift by 1.3mA). You won't have potential TLV431 stability issues to deal with either and it's cheaper!
A RED LED.
This is possible.
But why should I change? It works pretty wel with TLV431.
 
Why should I change C7. It seems doing the job.
It keeps the upper bandwidth to 900kHz, which is a good value.
Keeps giving a good oscilloscope wave.
My reply was to @brian92fs , as you can see from the order of the posts. BTW, you have no oscilloscope wave. You have a simulator wave. That is a big, big difference. You do not know how the real amplifier would behave.
 
Is 200mA a good value in the output or should I decrease it a bit?
Hitachi's laterals and their second sources have a Q point at which the temperature coefficient becomes 0 at around 120mA, so many DIYers set the value around that.
For FETs with square-law characteristics, the larger the bias current, the lower the distortion. At 200mA, the temperature coefficient is negative, so as long as the heat dissipation conditions are acceptable, there should be no problem.

But why should I change? It works pretty wel with TLV431.
However, the temperature coefficient is negative when the bias voltage is constant. In this circuit, the bias circuit is not a constant voltage circuit but just a resistor, so it changes in proportion to the quiescent current of the VAS.
It is recommended that the temperature coefficient of the VAS current is also close to 0 according to the advice of Bonsai.
Since the temperature coefficient of TLV431 is 0, it cannot cancel the temperature coefficient of U7.
 
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My reply was to @brian92fs , as you can see from the order of the posts. BTW, you have no oscilloscope wave. You have a simulator wave. That is a big, big difference. You do not know how the real amplifier would behave.
Of course you are very right.
Simulations are one thing - real amplifier a whole lot of different.
It is just that I have no real amplifier - so I have to use simulations.
 
This is a updated schematic. Number 15 ...
Changed a little bit the TMC compensation.
Repllaced TLV431 with two 1N4148 diodes in current sources.
Changed the optimal bias current in output. Now 173mA. Gives the lowest dist at 1 Watt output.
 

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For the IPS & VAS CCS, I ran some simulations on different configuration to see how it impacts slew rate. I tested 2 diode and feedback transistor style CCSs with the base stopper at the VAS or IPS side.

You can see that placing the base stopper on the IPS side improves negative slew rate and the feedback transistor version performs slightly better.

These sims were all ran with 20V rails with a 20KHz square wave at 1V peak
 

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For the RC caps R14 & R15, I don't think they need to be this high. I'd suggest dropping from 4700u to 470u. PSRR will still be good and PCB layout will be easier. 4700u caps can get quite larger.
Yes and not only. 4700uF on-board bypass capacitors are a source of current peaks that flow through the PCB ground tracks and as a result there is a raise of mains component multiples at the amp output. Just the opposite than the author wanted to have. Again, it is necessary to build prototypes to know this. Or to make much more complex simulations.
 
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For the IPS & VAS CCS, I ran some simulations on different configuration to see how it impacts slew rate. I tested 2 diode and feedback transistor style CCSs with the base stopper at the VAS or IPS side.

You can see that placing the base stopper on the IPS side improves negative slew rate and the feedback transistor version performs slightly better.

These sims were all ran with 20V rails with a 20KHz square wave at 1V peak
Thanks.
See the image.
Self uses IPS base stopper in his Blameless. And two diodes CCS..
 

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