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Is class A bass light?

It’s a more complex subject then you suggest - but the foundation of any amplifier is its PSU.

Presuming a "flat" frequency response amplifier there are some important parameters of an amplifier design that effect the perceived Bass performance.

1. Open loop output stage impedance (this is the OPS inherent output impedance before the application of Globe feedback).

2. Power Supply Rejection Ratio - its often erroneously assumed that PSRR will be equal or greater then the amplifiers FB gain – but this is not the case as PSU noise (Modulation) is often injected as Common mode and thus “Invisible” to the Feedback loop.

3. Open loop gain – the more gain the lower the Closed loop output impedance…

The Aleph30 and to a lesser degree the JLH 20W designs are poor in the above parameters making them very sensitive to there PSU performance – this does not need to be the case.

Sonically the JLH20W is still a “landmark design” – game changing for its time (WRT Transistors amplifiers of the day), but that was over 40 years ago - sadly few designs have advanced the art since (with a few notable exceptions such as the Quad Current Dumping)...

I never said was simple!
My Aleph used an overkill unregulated supply, my JLH used a regulated supply.
My favourite amps (and I have build many 10's) use single rail supplies - Nytech/Obelisk, valve amps, JLH. These need very careful execution to get the grounding right, but somehow sound more correct to me. Maybe it's because they have higher o/p impedance and Robert is right!
Of course there are still plenty of exceptions: e.g. Quad 909, NAP300 are fabulous amps.
 
As I understand it the Aura PA200 had reliability problems with the OPS and my units have had a redesigned module fitted. Maybe in overcoming the reliability issue it has had an effect on the low end control.

I am very happy with the natural open sound of the CDQ / AURA / Allison combination and do not feel it is missing any low end for my music tastes in my smallish study. I have been missing something from the Proacs up to now and the 8000P has brought them into line so if I want something a bit more punchy I can turn up the volume in that room.

Some things work well together and the trick is to find the right combination.
 
It’s a more complex subject then you suggest - but the foundation of any amplifier is its PSU.

Presuming a "flat" frequency response amplifier there are some important parameters of an amplifier design that effect the perceived Bass performance.

1. Open loop output stage impedance (this is the OPS inherent output impedance before the application of Globe feedback).

2. Power Supply Rejection Ratio - its often erroneously assumed that PSRR will be equal or greater then the amplifiers FB gain – but this is not the case as PSU noise (Modulation) is often injected as Common mode and thus “Invisible” to the Feedback loop.

3. Open loop gain – the more gain the lower the Closed loop output impedance…

The Aleph30 and to a lesser degree the JLH 20W designs are poor in the above parameters making them very sensitive to there PSU performance – this does not need to be the case.

Sonically the JLH20W is still a “landmark design” – game changing for its time (WRT Transistors amplifiers of the day), but that was over 40 years ago - sadly few designs have advanced the art since (with a few notable exceptions such as the Quad Current Dumping)...


Although it may seem counter-intuitive, in many applications (not in zero feedback designs obviously) your point 1 is not correct... I was quite surprised at the proof myself! It was shown by Prof. E. Cherry that in the case of both common collector (emitter follower) and common emitter output stages, that all being equal up to that point, when the feedback loop is closed the extra open loop gain of the CE OPS reduces the closed loop output impedance to exactly match that of the EF OPS..... ;)
 
Fan cooling appears to be the only practical means of realising class A amps of reasonable output without them becoming too massive or heavy in my experience. Noise issues can be dealt with by using oversize fans operating at a fairly low speed. The safety aspect needs thermal switches on the heatsink that will switch off the power if the fans fail and the temperature rises to dangerous levels.
Ah, that'll be the design flaw of the Musical Fidelity A-100 then. The fan-cooling had sucked household dust inside the hot bits, thereby progressively insulating them until they blew up from self-combustion. Clearly, there was no thermal switching ...
 
1. Open loop output stage impedance (this is the OPS inherent output impedance before the application of Globe feedback).

But we don't use amplifiers open loop, or listen to them like that.
What matters sonically is the end result, ie the performance taking into account the global feedback.

This is rather like looking at the localised performance of regulators in isolation, as is common especially for those offering aftermarket or add-on upgrades, without then examining the output of the device being powered for related effects.


IMaybe it's because they have higher o/p impedance and Robert is right!

Output impedance is the elephant in the room when it comes to amplifiers.
The one solitary specification difference among otherwise acceptably flat, low distortion amplifiers of sufficient power that will impact the sonics in often very audible ways - and predictably so if you have the full load spec.
You'd be surprised at how many clean and tight SS amps can sound remarkably tubey by simply inserting 4-6 Ohm resistors into the loudspeaker lines.... :)
 
Although it may seem counter-intuitive, in many applications (not in zero feedback designs obviously) your point 1 is not correct... I was quite surprised at the proof myself! It was shown by Prof. E. Cherry that in the case of both common collector (emitter follower) and common emitter output stages, that all being equal up to that point, when the feedback loop is closed the extra open loop gain of the CE OPS reduces the closed loop output impedance to exactly match that of the EF OPS..... ;)

I guess this is where we will have to differ, having to rely on FB to reduce output impedance does not result in the sonic performance as an output stage with “inherently” the same output impedance as would be obtained by the use of global feedback.

Effects that come into play is the reverse EMF from the speaker driver which does not see a true Zero ohm source – unheeded by the OPS poor impedance finds it way into the input stage of the amplifier thus upsetting the amplifier loop with an erroneous error signal (the phase of this back EMC is anyone's guess) - this is especially troublesome around the Class A/B crossover region where the output stage experiences severe impedance variations - the output stage is effectively “Open loop” (OK the loop gain is all over the shop) and feedback is at best struggling to act – transversing this region results in Phase error which is dependent (amongst other factors) on the ratio of the OPS “Real” output impedance and the load impedance. This is a classic example where global FB is not a cure for all ills.

Being a phase error - individual frequency components within a complex musical signal are affected to a greater or lesser extent – the PM having a greater effect on higher frequency components. As this Phase modulation effect is "non linear" across the audio BW phase coherence is lost during this critical part of the musical signal (Sound stage and "resolution" information is contained within the Low level signal region where output stages typically transverse “rapid” impedance variations).

Pure ClassA, Non Switching Class B designs (and other “Super” Class A derivates) do not suffer this effect - its also why its preferable to bias ClassA/B MOSFET designs (which do not suffer from GM doubling) heavily into ClassA operation in an effort to move this PM / impedance transition beyond the critical low level information region.

Over the past 1.5 year I've worked very heavily in developing the topology of our little MIMP amplifier which uses a Bootstrapped ClassA design - the Spice simulations clearly show the effects of back EMF and PM "amplified" by poor “real” output impedance (and the rapid impedance variations during the crossover region). Not only do these impedance variations open the “Gate” to back EMF reaching the input stage, it also allows the speaker cables conducted RF unheeded access to the input devices – which if bipolar junctions are only to happy to demodulate this RF energy with wild abundance…

Speaking for myself and my own design ethos, inherently low OPS impedance is critical on many levels – Global feedback should be considered a friend who’s helping hand should only be called upon in rare times of need…
 
also from my experience I'd say they can indeed lack ultimate bottom end "thump" - but have always found there midband to be very open and a very spacious sound stage.

I've always assumed the lack of very Tight Bass to be due to the higher Open Loop output impedance in the Mosfet output stage which can be 10dB to 20dB worst then an equivalent Bipolar OPS.

Interesting, I have never thought my MOSFET amps lacked bass but they use an error correcting technique described by Hawksford, I am sure you have seen it but here it is anyway for any one else who is interested.

http://www.essex.ac.uk/csee/research/audio_lab/malcolmspubdocs/J3 Distortion correction PA.pdf

Bob Cordell did an application note for Siliconix, I think!, that used this technique.
 
Interesting, I have never thought my MOSFET amps lacked bass but they use an error correcting technique described by Hawksford, I am sure you have seen it but here it is anyway for any one else who is interested.

http://www.essex.ac.uk/csee/research/audio_lab/malcolmspubdocs/J3 Distortion correction PA.pdf

Bob Cordell did an application note for Siliconix, I think!, that used this technique.

Well indeed :) - the OPS EC loop goes a very long way to resolving the above problems... well trimmed and your looking at atleast 40dB error cancellation...
 
Well indeed :) - the OPS EC loop goes a very long way to resolving the above problems... well trimmed and your looking at atleast 40dB error cancellation...

Certainly seems to work, some MOSFET designs can have an etched sterile quality and it seems to get rid of that too. I managed to measure a version of it once on an audio precision, unfortunately lost the results, but the results looked very good.
 
I guess this is where we will have to differ, having to rely on FB to reduce output impedance does not result in the sonic performance as an output stage with “inherently” the same output impedance as would be obtained by the use of global feedback.

Effects that come into play is the reverse EMF from the speaker driver which does not see a true Zero ohm source – unheeded by the OPS poor impedance finds it way into the input stage of the amplifier thus upsetting the amplifier loop with an erroneous error signal (the phase of this back EMC is anyone's guess) - this is especially troublesome around the Class A/B crossover region where the output stage experiences severe impedance variations - the output stage is effectively “Open loop” (OK the loop gain is all over the shop) and feedback is at best struggling to act – transversing this region results in Phase error which is dependent (amongst other factors) on the ratio of the OPS “Real” output impedance and the load impedance. This is a classic example where global FB is not a cure for all ills.

Being a phase error - individual frequency components within a complex musical signal are affected to a greater or lesser extent – the PM having a greater effect on higher frequency components. As this Phase modulation effect is "non linear" across the audio BW phase coherence is lost during this critical part of the musical signal (Sound stage and "resolution" information is contained within the Low level signal region where output stages typically transverse “rapid” impedance variations).

Pure ClassA, Non Switching Class B designs (and other “Super” Class A derivates) do not suffer this effect - its also why its preferable to bias ClassA/B MOSFET designs (which do not suffer from GM doubling) heavily into ClassA operation in an effort to move this PM / impedance transition beyond the critical low level information region.

Over the past 1.5 year I've worked very heavily in developing the topology of our little MIMP amplifier which uses a Bootstrapped ClassA design - the Spice simulations clearly show the effects of back EMF and PM "amplified" by poor “real” output impedance (and the rapid impedance variations during the crossover region). Not only do these impedance variations open the “Gate” to back EMF reaching the input stage, it also allows the speaker cables conducted RF unheeded access to the input devices – which if bipolar junctions are only to happy to demodulate this RF energy with wild abundance…

Speaking for myself and my own design ethos, inherently low OPS impedance is critical on many levels – Global feedback should be considered a friend who’s helping hand should only be called upon in rare times of need…

John. whilst you raise some valid issues (and a few tenuous ones), it's gone rather off topic to what you first said and to my reply! My point was merely that a high impedance OPS can have just as low an output z once the NFB loop is closed.... :)

There are as many opinions on some of the other matters you raise as there are engineers to voice them.... especially as to their relevance to overall results.... I guess this is why we all develop our own design ethos. It all helps to add variety to the subject anyway!
 
Pure ClassA, Non Switching Class B designs (and other “Super” Class A derivates) do not suffer this effect - its also why its preferable to bias ClassA/B MOSFET designs (which do not suffer from GM doubling) heavily into ClassA operation in an effort to move this PM / impedance transition beyond the critical low level information region.

Does it really need that much bias to avoid the issues you mention? I don't know much about amp design, but I'd have imagined so long as you are far enough away from the zero-crossing point for distortion to remain low, the NF must be working enough to keep output Z low too?
 
Ah, that'll be the design flaw of the Musical Fidelity A-100 then. The fan-cooling had sucked household dust inside the hot bits, thereby progressively insulating them until they blew up from self-combustion. Clearly, there was no thermal switching ...

Actually they did have a thermal switch. In spite of this fail-safe which would operate at about 90C, their normal operating temperature combined with standard 85C rated caps tended to eventually kill them off.... the A1 is just the same. I regularly carry out rebuilds on these models to bring them back to better than new electrical condition and the problems I find are usually heat related!
 
John. whilst you raise some valid issues (and a few tenuous ones), it's gone rather off topic to what you first said and to my reply! My point was merely that a high impedance OPS can have just as low an output z once the NFB loop is closed.... :)

I think what John is referring to is If the output device has not turned on, then the forward gain is zero and its a high Z output. That's why non switching, error correction and class A are preferred.
 
Does it really need that much bias to avoid the issues you mention? I don't know much about amp design, but I'd have imagined so long as you are far enough away from the zero-crossing point for distortion to remain low, the NF must be working enough to keep output Z low too?

Referring to MOSFETs here - typical rule of thumb is they like atleast 100mA pair device to keep there gain reasonably "Flat" about the crossover region which is quite gentle but also wide. I prefer to have this gradual variation then the abrupt crossover regions experienced with EF or even worst CFP Bipolor OPS.

Ideally you want to insure that the global feedback loop is always effective - as the output stage transverse the crossover region the global FB loop struggles to correct the error (the VAS can only compensate with its Open loop gain (hopefully the VAS has been adequately buffered from the non linear OPS loading effects about the crossover region) - but the output stage is not in a fit state to respond.

So in answer to your question, the idea is to move the OPS transitions point as far away from the critical Zero crossing point (MOSFET’s have the advantage as they don't suffer from the effects of GM doubling) as global feedback cannot be relied upon to correct the error (for ClassAB amplifiers).
 
I think what John is referring to is If the output device has not turned on, then the forward gain is zero and its a high Z output. That's why non switching, error correction and class A are preferred.

Thanks Russel - exactly what I was trying to explain :)
 
I think what John is referring to is If the output device has not turned on, then the forward gain is zero and its a high Z output. That's why non switching, error correction and class A are preferred.

Well that's just stating the obvious! Without enough forward bias to maintain conduction throughout the cycle then of course there will be a discontinuity where there is no loop feedback. Such an amp would be class B though and definitely not hi fi.... All this is totally irrelevant to my original argument though!

With an infinite open loop gain and zero phase shift an amplifier using NFB could give infinitely low distortion and zero output impedance (there are other ways of "faking" the later ;)) but in the real world this is of course impossible as that Nyquist geezer always comes in and spoils it.... it doesn't Bode well :)o)
Such an amplifier would work just as well at any bias setting as long as there was some forward bias, the NFB combined with the infinite gain would assure that.

Real world engineering is entirely about compromises and it is the choices available to a designer as to which compromises are the least pernicious that keeps the subject so exciting... and produces such a wide range of solutions to the age old problem of making small electrical signals loud enough to give listening pleasure!
 
Actually they did have a thermal switch. In spite of this fail-safe which would operate at about 90C, their normal operating temperature combined with standard 85C rated caps tended to eventually kill them off.... the A1 is just the same. I regularly carry out rebuilds on these models to bring them back to better than new electrical condition and the problems I find are usually heat related!
I stand corrected. My A-100 died a natural heat-related death within its first few years. The repair carried out by a tech made it sound noticeably inferior, so I moved it on.
 


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