CFA Topology Audio Amplifiers

Use of Cherry compensation results in much lower distortion at high frequencies(20 kHz) and insensitiveness to change of the bias current.

Simulation of the triple BJT OPS used beffore but compensation cap connected to the VAS output(classic Miller) instead to the amp output.
THD20k is 15 ppm at 120W/8ohm at optimum bias of 80 mA.

Compensation cap connected to the amp output(Cherry)
THD20k is 0.42 ppm at 120W/8ohm at optimum bias of 80 mA. This is 35 times or 30 dB lower. I never succeeded to get close to that result with the Hawksford EC(best was 20 dB) in my simulations.

With Cherry compensation THD20k was 0.83 ppm at the bias of 31 mA, 0.42 ppm at optimum bias of 80 mA and vent up to 1.04 ppm at bias of 340 mA.
That shows how the bias setting is not critical and even bias current fluctuation with increase of the output transistor is not critical.
BR Damir
 
"Square law rules".
Linear Audio volume 1, April 2011, p6-27 "Square law class A"
(that all the joy of Linear Audio, the authors seem not to have a limited number of pages to explain their investigations and circuits).

Not to rest on his laurels, Ian is now working on a 'cube law' error cancellation power amp, to appear in a future Linear Audio.
Class A all the way, but 1/4 of the idle dissipation 😉

Jan
 
Jan, I very much like Hegglun's works. I am a bit sad not to have read any comment about his article "Towards a reconciliation of measurements with listening tests" (Linear Audio volume 4) as it concerns both objective and subjective approachs to amplification.
 
This is of considerable interest, more details would be appreciated.
What was the approximate calculation?
What typical PCB trace inductance and capacitance did you arrive at?

Get this. Short free version here.

0.8mm width of 30um thick PCB trace on 1.6mm FR4 over a ground plane has 5.3nH/cm and 0.6pF/cm.

15cm of PCB trace resonate with 1pc of IRFP240 power mosfet Ciss (1300pF) at about 16MHz. With 5 IRFP240 in parallel, resonance is at about 7MHz. This is a very rough calculation, in reality the Ciss' are distributed across the PCB trace.

You have to use gate resistors that create poles in the forward path at significantly less than these resonance frequencies, to isolate them.
 
Last edited:
OPS local feedback implies multiple loops so you have to be very careful when you talk about "the" ULGF, because there are several.
In many practical implementations it is possible to find a Return Ratio that defines the stability of the entire amplifier and hence sensible to discuss "the" ULGF.
This is practically never the ULGF of the overall loop.
David

So piecing together my limited knowledge on the subject. This statement could be wrong. For two topologies, one with ops local feedback and one with only GNFB, both using the diamond front end and the same output devices the overall Return Ratios would be comparable. This is assuming similar specs for THD etc.

So your low overall amp ULGF here is almost irrelevant, unfortunately.
At least it provides a probable lower bound to the relevant ULGF, so not totally irrelevant.😉
As Waly correctly points out, this also applies to Damir's 1.7 MHz number.

Best wishes
David

See your point now. What a rookie error! But that's what I am unfortunately.
 
0.8mm width of 30um thick PCB trace on 1.6mm FR4 over a ground plane has 5.3nH/cm and 0.6pF/cm.

15cm of PCB trace resonate with 1pc of IRFP240 power mosfet Ciss (1300pF) at about 16MHz

so? use 8 mm wide trace - if you want RF performance you have to design with RF trace

http://www.ixysrf.com/index.php?pag...ategory_id=16&option=com_virtuemart&Itemid=35 ("only" 4.5 mm gate lead)

more on package parasitics: http://www.ixysrf.com/index.php?opt...ckages-in-high-speed-high-frequency-operation
 
Last edited:
I did.

1.7MHz is as relevant as the TMC loop gain analysis without breaking the connection to the output (hiding the fact that TMC is second order). Just another smoked mirror.

I think that you complicate to much, I used similar simulation for my VFAs with TMC and bult a few of them. All of them were very stable and good sounding. Did you ever build any real amp, if yes please show some to us please?
 
Agreed - that's exactly what my simulations showed on my TGM7 comparing VFA and CFA - as the OLG's are the same, the distortion profiles are pretty much the same. But I do like the practical advantage that for pcb layout, the low impedance feedback node is less susceptible to parasitic pick-up.

Even in a VFA I like to keep the feedback node impedance in the 250 to 500-ohm range. It is easy to do, but one must be aware of the dissipation in the feedback resistor when such low impedances are used.

Cheers,
Bob
 
Called
"quadratic class A" in France by Hephaistos / Gérard Perrot about thirty years ago
"curve linear class A" by Ian Hegglun.

Ian Hegglun published circuits using this kind of output stage in Elecronics World + WW, Sep 1995 p754-756, "Square law rules".
Linear Audio volume 1, April 2011, p6-27 "Square law class A"
(that all the joy of Linear Audio, the authors seem not to have a limited number of pages to explain their investigations and circuits).

There was also an interesting circuit proposed by Ian Hickman as an evolution of Pass's Zen in Electronics World, Aug 1999, p682, "New Zen".

Is "square class A" able to solve the main problems of output stages ?
What Bob Cordell said may apply to it :

Let's not forget the LT1166 chip, which implements essentially the same concept as the squre law approach, although I don't recall if it is mathematically identical. The LT1166 works well when properly applied, but such proper application is not really described in the app note. I do discuss it in my book. With the LT1166, neither output transistor ever completely turns off.

Cheers,
Bob
 
so? use 8 mm wide trace - if you want RF performance you have to design with RF trace

275-501N16A-00 ("only" 4.5 mm gate lead)

more on package parasitics: The destructive effects of Kelvin leaded packages in high speed, high frequency operation - IXYS Colorado

I'm afraid you quoted me out of context. This was about how many mosfets you can parallel until the law of diminishing returns apply.

With 8mm gate traces the resonance increases by a factor of 2.5. It also adds about 120pF of capacitance from the gate to the ground (it's actually in parallel with Cgd (of the same order of magnitude), for the upper half of the output stage).
 
For the use of the vertical MOSFET has a good article:
Stewart Edmond, Autobias for mosfet audio out stage, Electronics World 12/2003 p. 17-20
which shows that the field of vertical transistors tranzmstorov most complementarity Hitachi type 2SK1530/2SJ201 (2SK1529/2SJ200).
This is confirmed by research firm and National Semiconduktor AN-1645
I also conducted research with different FETs in the amplifier:
http://zalil.ru/34828511
and found that the popular and cheap type transistors IRFP240/IRFP9240 give a bad sound, although the parameters of the amplifier measured at work on resistive load high enough.


regards
Petr

There are many different ways to use the IRFP240/9240, and I'm not surprized if some of the designs do not sound good; this is true of most devices. I believe that they are capable of superb sound and measured performance at the same time.

Cheers,
Bob
 
so? use 8 mm wide trace - if you want RF performance you have to design with RF trace

275-501N16A-00 ("only" 4.5 mm gate lead)

more on package parasitics: The destructive effects of Kelvin leaded packages in high speed, high frequency operation - IXYS Colorado

I should note that I discussed vertical MOSFET resonances and parasitic oscillations in my MOSFET power amplifier with error correction article a long time ago. In that article I explained the use of gate Zobel networks to mitigate the problem. Dealing effectively with parasitic oscillations or instabilities in vertical MOSFETs without totally killing the HF performance with brute force gate stopper resistors is key to making the best use of verticals.

Cheers,
Bob
 
Thanks for this Waly. This is an excellent document and worth study on many fronts.

0.8mm width of 30um thick PCB trace on 1.6mm FR4 over a ground plane has 5.3nH/cm and 0.6pF/cm.

15cm of PCB trace resonate with 1pc of IRFP240 power mosfet Ciss (1300pF) at about 16MHz. With 5 IRFP240 in parallel, resonance is at about 7MHz. This is a very rough calculation, in reality the Ciss' are distributed across the PCB trace.

You have to use gate resistors that create poles in the forward path at significantly less than these resonance frequencies, to isolate them.
Wouldn't it be better to have ju..ust sufficient gate resistance AT the MOSFETs to critically damp the resonance?

This would introduce the least amount of evil phase shift. I don't think its sensible to try to isolate them. That would be a brute force solution.
Bob Cordell said:
I explained the use of gate Zobel networks to mitigate the problem. Dealing effectively with parasitic oscillations or instabilities in vertical MOSFETs without totally killing the HF performance with brute force gate stopper resistors is key to making the best use of verticals.
Bob, do you think gate Zobels can totally remove the need for stopper resistors?

My concern is that the Zobel introduces further 'capacitance'.
 
Last edited:
Ferrites work wonders here in the mosfet gate leads (also works for bipolars as well). There are cyclindrical types that slip over the device leads and you can also use the SMD versions. You need need to select the correct values though - I spent some time with a Murata kit a while back.
 
Thanks for this Waly. This is an excellent document and worth study on many fronts.

Wouldn't it be better to have ju..ust sufficient gate resistance AT the MOSFETs to critically damp the resonance?

This would introduce the least amount of evil phase shift. I don't think its sensible to try to isolate them. That would be a brute force solution.
Bob, do you think gate Zobels can totally remove the need for stopper resistors?

My concern is that the Zobel introduces further 'capacitance'.

No, the Zobels just reduce the amount of gate stopper resistance needed. I think I used 100 ohms for the gate stopper in the MOSFET amp with error correction.

Cheers,
Bob