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Please forgive me if this has been discussed ad-nauseum ..... . . . . .. . . . .Here's what i want to know: for any given length, is silver wire different than copper, in any kind of measurable or detectable degree?Yes, capacitance is a factor of diameter and dielectric. Given equal functions of each.Silver is the best conductor there is, that's plain physics in action. Unarguable. However, is copper linear in it's less-than-ideal-conductivity? and if so, does that characteristic impart any kind of measurable sonic signature?So, given interconnects and speaker cables, is the 'purity' of silver any different than copper: IE is copper's resistance non-linear enough to impart any kind of measurable or perceptive signature to the signal in comparison to a pure AG? Since copper is not the BEST conductor, is that 'non best' aspect of it linear and equal, or is there a response curve that's significant in any way?Just curious. I have a few hundred feet of pure 30AWG fine silver wire.......... Big deal or no?
Is it more conductive than gold, but with that juicy lack of corrosion?
So we find that the signal travels on the surface of the wire, and anything that is directly touching the surface will be introduced into the music.
I would try 1 24awg silver wire strand with natural unbleached cotton tubing. I tried the Teflon tubing (back and forth, switching the tubing out with cotton) and it killed the sound, also the teflon made it sound forward, harsh and the famous "bright" sound. So we find that the signal travels on the surface of the wire, and anything that is directly touching the surface will be introduced into the music. Teflon and PVC are synthetic materials, natural unbleached cotton is not, so maybe thats the reason why?I dont think about cables or upgrading or such anymore, this topology works and sounds the best for me and has for some years now.
I agree. I've had good results with Jupiter Condenser cotton insulated wire making a few diy ICs. I made one with 1 strand of 28g silver w/ a 20g magnet wire ground...
RAM is right about plastic insulators,by using cotton or silk "tubing" as an insulator you have something closer to air as a dielectric.
Be careful in how you twist the insulated conductors as the object when making a twisted pair or a braid is to have a uniform capacitance per foot avoiding wild variances in the capacitance over the length of the cable.
Quote from: DaveC113 on 6 Oct 2007, 04:23 amI agree. I've had good results with Jupiter Condenser cotton insulated wire making a few diy ICs. I made one with 1 strand of 28g silver w/ a 20g magnet wire ground...Should also have compared two strands of 28 gauge silver to two strands of the 20 gauge magnet wire.The whole notion of separate "signal" and "ground" doesn't really apply here. The signal doesn't propagate just down the "signal" wire. It propagates between the two conductors. It doesn't know "ground" from well... a hole in the ground. This also goes for the notion of a separate "send" and "return." The signal is AC. Current alternately flows in both directions in both wires. So half the time your "send" is a "return" and your "return" is a "send."se
If in fact cotton or silk has a higher dielectric constant in tubing form than teflon do you have a theory as to why a textile sounds better than a solid insulator when used to insulate a conductor in a cable.
I would still argue that a silk or cotton tubing will have a lower density of material and at least a certain amount of air next to the conductor than a solid plastic.
As far as the uniformity of geometry is concerned,I would say the jury is still out on that one. If the audio signal only sees the lump capacitance of the cable than the sound staging could be manipulated via a simple addition or subtraction of a capacitor across the cable from hot to ground. This has not been the case in my experience. The bandwidth of the connection between the two devices,ie [a DVD player and a preamp] is dependent on the filter pole defined by the RL plus the lump capacitance but dismissing the importance of the cable geometry and its relationship to how the cable sounds is an over simplification.
As far as AdamM is concerned, I fear that the discussion has gone beyond the requirements necessary for a simple experiment with DIY cabling and into the realm electrical theory. AdamM can determine what works for him with some empirical trail and error and have some fun along the way.