No, didn't forget directionality it at all, it doesn't matter. Audio signals are not truly symmetrical or balanced (plus to minus signal don't subtract to zero) as impulse noises are more positive amplitude than the negative decay. Look at a piano or drum strike, for instance. Yep, more stuff on the positive side than the negative side. But this is no reason to think the "positive side" needs help.
The waveform is alternating current and travels BOTH directions with respect to polarity. What half of the waveform do you want to be biased with the copper "grain" structure? If this was a DC signal, rubbing against the copper grain structure the wrong way may be a fun FUD argument. But since audio cables aren't a cat and get pissed when rubbed the wrong way and are AC in nature, this concept of current "direction" when it has reversal changes to even play music is rather odd.
I already discussed polarity reversal timing (fast as the dickens) in the dielectric relative to single directional changes. How on earth could AC signals even be transmitted if the dielectric were "slow"? Coaxial cables transmit in the 6 Gig frequency range all day with out directionality just fine, thank you. And, their dielectrics don't need help...
DC dielectric bias systems are also perplexing. DC bias systems further tell you that the signal could care less about directionality and polarity as a DC bias system theoretically makes it HARDER to polarize in the opposite direction of the bias. All good dielectrics polarize so fast that a DC impediment doesn't audibly affect the sound, just your pocket book. Why so much concern for the BIAS in the ONE direction only? And no, a dielectric doesn't take seconds, minutes, hours or days to polarize. It takes 10 to the minus fourteen seconds. Do they wander around after power is removed? Yes. Do they snap back into control IMMEDIATELY when a signal is applied? Yes. If you listen to music at the 10 to the tenth power in frequency...be worried, very worried, as the polarization can now not keep up. So how does a DC battery bias system add speed to an audio signal dielectric and to both polarities, not just one?
But if you must, mark your cable and add an arrow to make you feel good along with a battery and heavens don’t put the battery in the wrong direction! :)
I'm not against REAL design metrics that is repeatable and you can design around. To jump to RF wave-guide signals and force an issue at audio is simply misguided. Audio cables are hard enough without using physics the wrong way.
All the attributes I discussed are measurable at audio, and the improvements to them rational in a good design. Diectionality, DC bias and many others are not. But if you want to add nonesense to cables, why not add it to a cable that at least is designed right up to the arrows and battery installation steps? Are we tossing out what we can measure and replacing it with what we can't? Yep, we see pages of FUD "data" (differentiation)with no mention of the compliance to the physical basics. If a cable meets the basics, at least the FUD stuff didn't hurt the sound, just your pocket book.
The waveform is alternating current and travels BOTH directions with respect to polarity. What half of the waveform do you want to be biased with the copper "grain" structure? If this was a DC signal, rubbing against the copper grain structure the wrong way may be a fun FUD argument. But since audio cables aren't a cat and get pissed when rubbed the wrong way and are AC in nature, this concept of current "direction" when it has reversal changes to even play music is rather odd.
I already discussed polarity reversal timing (fast as the dickens) in the dielectric relative to single directional changes. How on earth could AC signals even be transmitted if the dielectric were "slow"? Coaxial cables transmit in the 6 Gig frequency range all day with out directionality just fine, thank you. And, their dielectrics don't need help...
DC dielectric bias systems are also perplexing. DC bias systems further tell you that the signal could care less about directionality and polarity as a DC bias system theoretically makes it HARDER to polarize in the opposite direction of the bias. All good dielectrics polarize so fast that a DC impediment doesn't audibly affect the sound, just your pocket book. Why so much concern for the BIAS in the ONE direction only? And no, a dielectric doesn't take seconds, minutes, hours or days to polarize. It takes 10 to the minus fourteen seconds. Do they wander around after power is removed? Yes. Do they snap back into control IMMEDIATELY when a signal is applied? Yes. If you listen to music at the 10 to the tenth power in frequency...be worried, very worried, as the polarization can now not keep up. So how does a DC battery bias system add speed to an audio signal dielectric and to both polarities, not just one?
But if you must, mark your cable and add an arrow to make you feel good along with a battery and heavens don’t put the battery in the wrong direction! :)
I'm not against REAL design metrics that is repeatable and you can design around. To jump to RF wave-guide signals and force an issue at audio is simply misguided. Audio cables are hard enough without using physics the wrong way.
All the attributes I discussed are measurable at audio, and the improvements to them rational in a good design. Diectionality, DC bias and many others are not. But if you want to add nonesense to cables, why not add it to a cable that at least is designed right up to the arrows and battery installation steps? Are we tossing out what we can measure and replacing it with what we can't? Yep, we see pages of FUD "data" (differentiation)with no mention of the compliance to the physical basics. If a cable meets the basics, at least the FUD stuff didn't hurt the sound, just your pocket book.