"You are correct about skin effect. Skin effect is a phenomenon that you tend to see at microwave frequencies."
This is incorrect. At microwave frequencies skin depth is in order of um. At audio frequency of 20kHz largest copper wire that has still the same resistance for DC as AC is gauge 18. Please check skin depth calculator here:
http://daycounter.com/Calculators/SkinEffect/Skin-Effect-Calculator.phtml
Skin effect is very pronounced at video frequencies. That's why cables are made of cheap metal silver plated (signal travels on the surface).
Skin effect allows for shielding. Interconnect for instance cannot be possibly protected from electromagnetic pickup of high frequency signals by non-magnetic shield. What really happens is that shield passes these high frequencies and they are induced in the cable, but because of skin effect they travel on the outside of the cable - shield. Internally field is zero as long as wire is symmetrical. Without skin effect aluminum foil or copper braid would not shield higher frequencies (would protect only for capacitive pick-up). Shielding is very complicated. Shield is carrying externally induced high frequencies on its outside while at the same time common mode high frequency signal noise travels on the inside of the same shield. At lower frequencies shield does not protect at all but wire is to short to become effective antenna (starts at 1/10 of wavelength)
Audio cables are much more complicated than just RLC. If I remember correctly Muralman1 uses in his design cable different metals for signal and Ground wires. You cannot explain in terms of RLC how different metals change the sound.
This is incorrect. At microwave frequencies skin depth is in order of um. At audio frequency of 20kHz largest copper wire that has still the same resistance for DC as AC is gauge 18. Please check skin depth calculator here:
http://daycounter.com/Calculators/SkinEffect/Skin-Effect-Calculator.phtml
Skin effect is very pronounced at video frequencies. That's why cables are made of cheap metal silver plated (signal travels on the surface).
Skin effect allows for shielding. Interconnect for instance cannot be possibly protected from electromagnetic pickup of high frequency signals by non-magnetic shield. What really happens is that shield passes these high frequencies and they are induced in the cable, but because of skin effect they travel on the outside of the cable - shield. Internally field is zero as long as wire is symmetrical. Without skin effect aluminum foil or copper braid would not shield higher frequencies (would protect only for capacitive pick-up). Shielding is very complicated. Shield is carrying externally induced high frequencies on its outside while at the same time common mode high frequency signal noise travels on the inside of the same shield. At lower frequencies shield does not protect at all but wire is to short to become effective antenna (starts at 1/10 of wavelength)
Audio cables are much more complicated than just RLC. If I remember correctly Muralman1 uses in his design cable different metals for signal and Ground wires. You cannot explain in terms of RLC how different metals change the sound.