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Indeed persistent attempts by solid state designers to clone the very unique manner in which vacuum tubes affect the audio signal by using simple tone networks have always been a laughable and dismal failure.
Maybe, but using the correct method, it has been a success. The tweaked transistor amplifier could not be distinguished from the tube one. Does someone have the reference of this experiment ?
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While the "first order" effects of LC influenced frequency attenuation are well characterized, indirect effects of their time delay components on our perception of the more subtle aspects of playback are not.
Yes they are. 2bdecided or Wmax must have some tables in their documentation adout the smallest phase shift audible under different conditions.
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One or two degrees of phase shift can be calculated in the audio band from capacitance whose frequency attenuation is well into the ultra-sonic regions. Exactly what one degree of phase shift and perhaps one tenth of a dB of attenuation may sound like is not known and is probably very unpredictable and extremely dependant on the particular source material.
They effect is very predictible and perfectly known : this is not audible at all.
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Such small effects could not normally be seen since they would be hidden in the noise floor of measuring equipment. Instead actual their existence can only be suggested mathematically.
This is completely wrong. With a PC, a good soundcard, and the RMAA software, you can measure frequency attenuation down to 0.01 dB. That can be seen on the interconnect cables frequency measurments I've done here :
http://www.homecinema-fr.com/forum/viewtopic.php?t=29781210QUOTE
The fact that different audio cables do affect system performance differently would be especially challenging to defend if all audio cables had identical LC measurements. Luckily, this is not the case, as different interconnect and speaker cable designs result in easily measurable variations in capacitance and inductance respectively. Aside from the resulting differences in phase shift by degree, placed into the big picture of impedance, seemingly modest differences in LC measurements calculate to substantial differences in impedance (frequency variant) and characteristic impedance (frequency invariant) especially with speaker cables. Measurable differences in amplifier damping (which produces a rainbow sonic aberrations to the listener) have been easily demonstrated with different speaker cable designs, all of whose direct effects on frequency response alone should have been inconsequential!
The amplifier damping only affects the frequency response, if I'm not mistaken, and as I said, only cables badly designed on puspose exhibit this effect. Standard speaker and interconnect cables don't affect the sound. They are completely transparent.
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Furthermore, with the exception of digital cables, no audio interconnect or speaker cable can be terminated in their exact characteristic impedance
That's right.
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a condition that theoretically results in 100% power transfer (zero power loss)
That's wrong, you're forgetting the DC resistance.
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Therefore, all audio cables create some degree, though very slight, of so called "mismatch reflections" between source and load.
That's right, but since the cables are thousand times shorter than the electrical wavelenght, these reflections can be discarded.
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It is then reasonable to assume that audio cable designs that happen to come closer to an ideal impedance should in principle reduce these distortions.
The ideal impedance is the impedance, from this point of view, of the speaker, which can't be reproduced by the characteristic impedance of a cable. But the point is that thanks to the low output impedance of the amplifier, and the relatively high impedance of the speaker, compared to the amplifier and the cable ones, even if these reflections would pollute the signal inside the cable, it would not affect the signal fed inside the speakers, thanks to the complete impedance mismatch between the three component (ampli, cable, speaker).