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Thank you John.So regardless of AWG of wire a single zip wire will have an impedence between 150-200?Is it per feet ?I was thinking of using Goertz M1 (http://www.goertzaudio.com/contents/en-us/d16_MI_Speaker_Cables.html) instead of DYI wire since it has the lowest inductance value I know.I just noticed that the Impedence is 4. So I was planning to use Goertz M1 for HF and ZIP cord for LF since the capacitance of Goertz cable is 500pF /feet . But from this discussion it seems like Zip cord even with low capacitance offers higher impedence.But going back to wikipedia the capacitance affect LF (copied from wikipedia) This table shows the capacitive reactance in ohms (higher means lower loss) for various frequencies and capacitances; highlighted rows represent loss greater than 1% at 30 volts RMS:The voltage on a speaker wire depends on amplifier power; for a 100-watt-per-channel amplifier, the voltage will be about 30 volts RMS. At such voltage, a 1% loss will occur at 3,000 ohms or less of capacitive reactance. Therefore, to keep audible (up to 20,000 Hz) losses below 1%, the total capacitance in the cabling must be kept below about 2,700 pF.Ordinary lamp cord has a capacitance of 10–20 pF per foot, plus a few picofarads of stray capacitance, so a 50 foot run (100 total feet of conductor) will have less than 1% capacitive loss in the audible range. Some premium speaker cables have higher capacitance in order to have lower inductance; 100–300 pF is typical, in which case the capacitive loss will exceed 1% for runs longer than about 5 feet (10 feet of conductor).I am not sure at this point should I be looking at impedence of the wire vs each reactance seperate?
The industry needs to meld localization theory with actual t-line theory, and actually learn how to measure high slew currents in low z systems.
So then, it is your assertion that an impulse plot of pink noise will clearly show a midband delay of anywhere from 5 to 50 microseconds? (actually, we are sensitive to 1.2 uSec interchannel, but that is a discussion beyond the scope of the forum in terms of image stability)..
And, if a switch is made from normal to biwire, that the composite soundfield modifications which result from driver to driver timing changes and consequent polar pattern changes in the 5 to 50+ microsecond range will be seen by a microphone?
ps. Until the "industry" actually learns this stuff, nobody's gonna accurately measure anything along these lines. That is why I mentioned the audibility test before. If it discerns an audible difference in the mono setup, there may be one at the stereo level. If not audible in the mono situation, there cannot be one in the stereo case.
I could imagine why they would believe that. Kinda inferred from "inherent cable velocity"
Which industry? The Audio industry needs to measure the acoustics and psychoacoustics of reproduction; otherwise they risk inventing problems to solve and ignoring real ones in the process.
Assuming a triangle is a line to make the math easier, and using 2ns, that would mean that we were sensitive to movement of a sound source of 1/563-millionth of a foot. That would cause 2 uSec change in arrival time of sound.
Or does the slew need to be between frequency X and frequency Y (rather than L/R, which is what I presently understand from you)... in which case it could be reproduced with that move in driver spacing. Perhaps loosen a screw imperceptibly.
Yea. I need to get to the store, grab some disposable wire and spend some time with that test. I have no good excuse, it's a practical test (with an admittedly impractical wire), but that I'm a procrastinator and it's functionally work.
Then you are also part of the "problem" so to speak.
The audio industry need to learn what it is the high end people are speaking about. While measurement is great, I see little actual understanding in localization theory nor transmission line theory. All I see is approximations.
What level of interchannel and intrachannel accuracy is required to stabilize virtual images in a +/- 60 degree soundfield generated by two speakers at +/-60 degrees. IOW, what level of ITD and IID control is required. And what level of change control in the wire impedance is required to allow that control between the amp and the load when the load impedance varies an order of magnitude?
To wit: this gem..2 nSec is the inherent propagation velocity of a cable with an effective dielectric constant of 4.2 uSec is the level of ITD humans are capable of resolving.Not a bad question. But you are using the head in vice argument, that is far too simplistic and inaccurate for the discussion.
I don't think you understood what I said.
They really don't. They need to understand what changes make perceptible improvements in the desirability of their products.
The end result of everything you are discussing is that the sounds appear with a relative delay (L vs R, 100Hz vs 1000Hz, etc), yes? Wire X has one set of delays and wire Y has another set. What is the order of magnitude for this delay?
I suspect we can find other things that introduce similar amounts of delay, such as driver alignment. That would give us something in real, widespread use we could judge by.
If I have to use a Zobel with Goertz what should be the component values I should use. Found an interesting article. http://www.audioholics.com/reviews/cables/speaker-cable-reviews-faceoff-2/speaker-cable-reviews-faceoff-2-page-3They recommend using 4.7ohm ,0.1uf for Zobel. Since I am DIYing it I thought I would include it. What type of resistor and capacitor I should go for?
Thanks John.I thought in the arguments going on you ignored this low Fi man. I read further and looked at Goertz site ,they actually have a Zobel at an exotic price of course, apparently built using regular components?The link in my last post describes how their zobel was not good in the testing but will work just as fine.I tried with braiding up two zips and found a difference in sound. I would describe it as instruments and voice seperated out in a nice way(more space) after braiding the zip to HF and some difference in Bass but I would say it is more in my brain since the second person, my friend who listened to could not appreciate a difference in bass. So I thought about doing this two type wiring for biwiring. PS:John I PM you some stupid questions. If I am not annoying you please be kind enough to send me a reply.
It's great that you are trying things. Remember though, it is very very difficult to be sure that what you are hearing as different is reality. Nature of the beasts we are is that expectation bias is there to be considered. Given all the variables in the systems as well as in the human, it is not really possible to analytically guarantee that any of these changes will rise to the level of repeatable audibility. I can guarantee that the changes are not zero however.. While all the market verbage out there may try to explain some kind of weird science to justify their product, the only differences for speaker cables will be L, R, C, and length. I've provided the simple math and science to allow the diy'er to experiment with different L and C combinations while not breaking the bank. If you come up with a combo that you like, just keep it.jnps..I do not recommend using a low impedance cable for the woofer side of a bi wire or even for a bi amp system. The cable will look like a capacitor when the woofer unloads at higher frequencies by design, and that may be troubling to an amp. You'd need a lower frequency zobel in that case, and the delays that the cable mismatch causes at bass are inconsequential as a result of our lack of phase sensitivity at lf.
Found something interesting from Vanderstein about biwiring.From Audioquest And this article (http://www.synergisticresearch.com/tesla-series/integrated-frequency-transmission-ift-a-better-way-to-bi-wire/ ) for using two different typeAnother method of bi-wiring is to run two different cables in parallel, thus giving the amplifier the ability to choose separate cables that are especially suitable for each half of the frequency range. This has been a hallmark of Synergistic Research cable design, going back to our fist Signature speaker wire: The Signature No. 2. If you assume that the signal always takes the path of least resistance, the right path will be chosen automatically"
You make sense to me. If I had the specs of my amps and crossover could a cable be designed to mate with them ? What would one need to know to do that ? As a Scientist you think differently than us audio guys. I appreciate and understand your position. WE listen you measure.
A pet peeve of mine is that the manf. does not offer specs for cables requirements related to their gear.
I am finding after few hours of listening that PTFE defenitely makes a difference in sound quality for good. And yes I do not think ,I burned in or anything, it just happened over few hours (4-6) of listening over last week.I found an explanation here http://www.empiricalaudio.com/computer-audio/technical-papers/dielectric-absorption-dissipation-factor-and-qIt was expensive compared to DIY using PVC wires from parts express but I am happy with it. Still using Zip cord for LF and braided PTFE 18AWG for HF. this weekend I will switch back to monowire with PTFE and see which one I like more.Capacitance measured is around 50pF /feet for braided wire,sorry no inductance meter. But according to Jneutron's theory it should be low.The lower capacitance might be from using PTFE insulation with low dielectric constant I assume.(3rd to air and second to cotton)I am planning to make two more pairs with PTFE for biwiring both speakers to see the difference. Will keep you posted.