Hello!
When comparing transistor and tube amplifiers, the significantly higher damping factor of the transistor amplifier is presented as a major advantage. I began to doubt this for some time. I designed and tested an audio current amplifier. Here is the functional description:
This amplifier drives a guitar speaker or a full-range speaker flawlessly. Meanwhile, its damping factor will be practically zero. So I started thinking, why is there something wrong with the theory? Finally, simulation with LTspice gave me the answer (at least I think so).
I found a model for the guitar speaker here: http://tamivox.org/dave/speaker/graphs.html
The test setup looks like this:
V1 is the ideal voltage amplifier with the infinitely large damping factor. Therefore, its output voltage does not depend on the load and can be loaded as desired. The current through the Rref can show us an ideal current pattern. Now the first measurement:
Surprisingly, the after-oscillations from the current amplifier have a much smaller amplitude than the after-oscillations from the voltage amplifier... Why?
Because the output voltage of the current amplifier counteracts the voltage induced in the loudspeaker coil and prevents the first huge swing as is the case with the voltage amplifier.
Furthermore, this exactly matches my listening experience. This sound is cleaner than the sound of my (standard) hi-fi stereo system.
When comparing transistor and tube amplifiers, the significantly higher damping factor of the transistor amplifier is presented as a major advantage. I began to doubt this for some time. I designed and tested an audio current amplifier. Here is the functional description:
This amplifier drives a guitar speaker or a full-range speaker flawlessly. Meanwhile, its damping factor will be practically zero. So I started thinking, why is there something wrong with the theory? Finally, simulation with LTspice gave me the answer (at least I think so).
I found a model for the guitar speaker here: http://tamivox.org/dave/speaker/graphs.html
The test setup looks like this:
V1 is the ideal voltage amplifier with the infinitely large damping factor. Therefore, its output voltage does not depend on the load and can be loaded as desired. The current through the Rref can show us an ideal current pattern. Now the first measurement:
Surprisingly, the after-oscillations from the current amplifier have a much smaller amplitude than the after-oscillations from the voltage amplifier... Why?
Because the output voltage of the current amplifier counteracts the voltage induced in the loudspeaker coil and prevents the first huge swing as is the case with the voltage amplifier.
Furthermore, this exactly matches my listening experience. This sound is cleaner than the sound of my (standard) hi-fi stereo system.