>>we develop a totally new mathematics theorem to make the transistor full linear<<
What kind of fluff is that? I'm not familiar with any of your designs, but coming up with some new equations on paper does not change the laws of physics. Active devices follow certain behaviors and have been well established. On one end of the scale is the triode, the most inherently linear amplification device used in audio. At the other end is the bipolar transistor (ok, maybe an IGBT is worse). In the middle are JFETs, pentodes, MOSFETs.
The bipolar transistor has a nearly perfect logarithmic transconductance. Hard to beat in that respect. But exponential is not proportional (linear). No theorem is going to change that.
If you have, however, invented some new circuit topology that does what you claim, then I suggest you patent it immediately. Silicon Valley is going to pound your door down.
>>more SS designs come with NON feedback design<<
Well, I think this is a little exaggerated. Most SS designs on the market employ opamps. Only a handful use open loop discrete gain stages. Perhaps this number is growing, but I hardly think it is dominant.
>>It is untrue that there is a technical limitation topology<<
What I didn't make clear here was the basic difference between class A and class B stages. As far as I know virtually all opamps run class AB. The output signal is driven in one direction by one device (transistor), and in the other direction by a second device. They keep handing off the signal. Only during a small crossover window do they both conduct. Making this window larger can help. Making the window full scale turns the amplifier back into class A. No device ever turns off.
In contrast, a class A stage is driven by a single device. It is always on. There is no cross over or handoff. This is the difference between a 2A3 SET and your typical SS amplifier. Why is it people will live with a flea-powered 2A3 when they can have 50 watts out of an LM3875 power opamp? Because of the micro detail. The SET is running full bore at idle. It excels at small signals and the distortion becomes vanishingly small. By comparison, the class AB amplifier excels at large signals. But it's distortion rises as the signal gets smaller. Exactly the opposite of the 2A3. That is an example of topology.
There are a lot of other topologies I can get into, but that example illustrates the point well.
>>tubes are harmonic generators<<
Yes. So is feedback. And the harmonics generated by feedback are far more insidious. They might be quite small in relative amplitude, but multiply with each pass through the amplifier, generating a lot of non-integer harmonics. That leads to the cold, sterile, and sometimes fatiguing sound of many high feedback amplifier stages.
SS stages that do not use feedback are also harmonic generators. Heck, every amplifier is to some degree. The question is, what sort of harmonics do you want to live with? I'll take a triode any day.
jh
What kind of fluff is that? I'm not familiar with any of your designs, but coming up with some new equations on paper does not change the laws of physics. Active devices follow certain behaviors and have been well established. On one end of the scale is the triode, the most inherently linear amplification device used in audio. At the other end is the bipolar transistor (ok, maybe an IGBT is worse). In the middle are JFETs, pentodes, MOSFETs.
The bipolar transistor has a nearly perfect logarithmic transconductance. Hard to beat in that respect. But exponential is not proportional (linear). No theorem is going to change that.
If you have, however, invented some new circuit topology that does what you claim, then I suggest you patent it immediately. Silicon Valley is going to pound your door down.
>>more SS designs come with NON feedback design<<
Well, I think this is a little exaggerated. Most SS designs on the market employ opamps. Only a handful use open loop discrete gain stages. Perhaps this number is growing, but I hardly think it is dominant.
>>It is untrue that there is a technical limitation topology<<
What I didn't make clear here was the basic difference between class A and class B stages. As far as I know virtually all opamps run class AB. The output signal is driven in one direction by one device (transistor), and in the other direction by a second device. They keep handing off the signal. Only during a small crossover window do they both conduct. Making this window larger can help. Making the window full scale turns the amplifier back into class A. No device ever turns off.
In contrast, a class A stage is driven by a single device. It is always on. There is no cross over or handoff. This is the difference between a 2A3 SET and your typical SS amplifier. Why is it people will live with a flea-powered 2A3 when they can have 50 watts out of an LM3875 power opamp? Because of the micro detail. The SET is running full bore at idle. It excels at small signals and the distortion becomes vanishingly small. By comparison, the class AB amplifier excels at large signals. But it's distortion rises as the signal gets smaller. Exactly the opposite of the 2A3. That is an example of topology.
There are a lot of other topologies I can get into, but that example illustrates the point well.
>>tubes are harmonic generators<<
Yes. So is feedback. And the harmonics generated by feedback are far more insidious. They might be quite small in relative amplitude, but multiply with each pass through the amplifier, generating a lot of non-integer harmonics. That leads to the cold, sterile, and sometimes fatiguing sound of many high feedback amplifier stages.
SS stages that do not use feedback are also harmonic generators. Heck, every amplifier is to some degree. The question is, what sort of harmonics do you want to live with? I'll take a triode any day.
jh