- Thread Starter
- #21
Aliens... On the Internet, nobody can hear you scream...
I'd forgotten how pompous some of these articles sound... A lot of them are going on ten years old as well so some references may be out of date.
Yes, skin depth says how much of the conductor will be used, and especially at LF the penetration depth is more reasonable. Pipes, e.g. conductors that are hollow on the inside (e.g. used for high-power transmission systems), are another special case since the EM fields are constrained in the center. Disclaimer: My last EM courses were decades ago so don't ask me to explain that stuff.
Using an ideal inductor as a first-order model with a series R equal to the DCR will get you in the ballpark. Modern simulators allow you to curve fit and/or create a nonlinear inductor that is a better fit. BUT, I have found that to be important at RF/mW/mmW; not so much at audio (where I normally ignore skin effect anyway).
For speaker cables, the often-neglected factor is what impedance the crossover sees. The problem IME with long speaker runs and/or small wires is the impedance rises enough that the crossover no longer sees a near-perfect voltage source and that cause frequency response variations. Very obvious in tube outputs, which tend to be fairly high anyway, but long speaker runs can shift the frequency response as well. Most designers, I am led to believe, use pretty good amplifiers that have very low output impedance. I have also seen the opposite, where the speaker designer used a tube amp for his reference, and a SS amp then provided a different frequency response. And so it goes...
Aside: We undoubtedly share a cross section of friends in and out of ADI. My main career until about ten years ago was designing high-speed data converters and other analog/mixed-signal ICs.
(DC Resistance is per 1000 feet or alternatively in milliohm):
I looked at several of these cables also, and reached an essentially identical conclusion- and no, I don't have my notes, but I do have some pretty decent test gear for this kind of situation, so I'm confident in the result.This is puzzling ... ELECTRICAL, house and building wire, has the "same" resistance for a given gauge whether standard 7 strand, fine 19 strand, extra fine 37 strand or something else stranded or solid. Stranded is larger in diameter because of air space, but that doesn't effect its resistance.
What I don't get is what this stuff is that you measured. 12AWG copper wire (solid or stranded) has a resistance of about 1.6 ohms/1000 feet. 12AWG aluminum wire has a resistance of ABOUT 2.6 ohms/1000 ft. Copper coated aluminum, depending on the copper thickness, will be between the 2. Anything outside that range (ignore the coat hanger) is suspect.
12AWG weighs about 30 kg/km ... single conductor, no insulation ... your weight measures, excepting the Southwire (yeah, you said similar to that spool) are probably for the cable, 2 (4 for the Canare) insulated conductors in an overall sheath.
Can I politely say I doubt your measurements? This was a year ago so perhaps you don't have any notes?
Using many small wires that are individually insulated makes up for the increased impedance that would otherwise be there and deals with skin depth at the same time, that is to say litz wire is not necessarily an unacceptable option for speaker wires.The problem IME with long speaker runs and/or small wires is the impedance rises enough that the crossover no longer sees a near-perfect voltage source and that cause frequency response variations.
One should, unless one is desirous of enstupidation.one should not dismiss Paul McGowan out of hand, because a lot of things he says are true.
Nope, I have watched a lot of his YouTube videos and found invaluable information. This wanton neglect for the perspective of some audiophiles is probably the reason why some don't like to participate in this forum. By the way, I looked your word enstupidation up and it's not a real word?One should, unless one is desirous of enstupidation.
I love the cite to a totally irrelevant article about RF amps.
Enstupidation is a perfectly cromulent word.Nope, I have watched a lot of his YouTube videos and found invaluable information. This wanton neglect for the perspective of some audiophiles is probably the reason why some don't like to participate in this forum. By the way, I looked your word enstupidation up and it's not a real word?
The quote was about the wiki article speaking on when parasitic capacitance kicks in. I was hoping someone can elaborate on whether parasitic oscillation is really only a problem at more than 500 kHz. Granted that I don't have the faintest idea about how to understand the RF amp article and merely thought it is interesting.
So who is really the reliable source here if you write some word that can't even be verified and you write something that is irrelevant?
Thanks. I understand now. Glad to learn English from native speakers on the Internet and pick up invaluable information about my entry into hi-fi along the way.Enstupidation is a perfectly cromulent word.
Here's the valuable advice:Thanks. I understand now. Glad to learn English from native speakers on the Internet and pick up invaluable information about my entry into hi-fi along the way.
I'm happy to embiggen your vocabulary.Now I also have to look up cromulent!
Keith
Seems like the perfect word for certain... eh.. phallic.. advertisementsembiggen
Ambiguous comment at its best. Could mean you prefer the skin effect. Could also mean you like litz-type wire that actually has more "skin". I wrote that litz wire is a way to deal with skin effect if one wants, but the difference in impedance is not that great.The best part of fried chicken is the skin.
You didn't mention anything about litz wire, but talked about the problem with impedance on small wires. So I commented on that. I for one think that your article here is not a waste of time.Posting articles here is clearly a waste of time.
You didn't mention anything about litz wire, but talked about the problem with impedance on small wires. So I commented on that. I for one think that your article here is not a waste of time.
Turns out buying 18 gauge insulated copper wires and twisting 2 together to make one 16 gauge speaker wire is even the cheapest deal I have found and deals with the little loss in energy from skin effect, which is nice.
I did not notice that, because I just did a cursory conversion from 0.75 mm² and 1.5 mm² that are the measurements used in Denmark. Turns out those numbers are in between the AWG values.Two 18 AWG wires in parallel actually yields about 15 AWG if you want to get picky, a hair better than 16 AWG. You gain about 3 AWG for each doubling.
I overlooked that you did mention litz wire, but not in detail.Here is an article about skin effect: https://www.audiosciencereview.com/...cle-does-audio-cable-skin-effect-matter.7157/