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Author Topic: Conductance in different materials.  (Read 6264 times)

danlavry

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Re: Conductance in different materials.
« Reply #15 on: February 03, 2005, 08:38:51 PM »

Sahib wrote on Thu, 03 February 2005 11:33

danlavry wrote on Wed, 02 February 2005 19:24



Say you have an 100 feet of an 18 gauge wire. The DC resistance is about 0.65 Ohms. The K factor for 18AWG wire is about 11. So the AC resistance is:
At DC .65 Ohms, at 20KHz it will become 1 Ohm, at 100KHz, 2.25 Ohm, at 1MHz we have 7 Ohms, 22 Ohms at 10MHz…

So yes, you may not want to use 100 feet of 18AWG for the speakers, but 10 feet is (0.1Ohm) probably fine, from skin effect standpoint. A 10AWG at 10feet yields DC resistance of 1 milliohm and with skin effect it comes to 4 milliohms, so even 100 feet of 10AWG is only 40 milliohms at 20 KHz (it is really 50 feet each direction).
 



Dan,

Many thanks for this. Yes the formula book I have has limited info on this issue. Can you recommend me a better one? What do you use?

Regards,
Cemal




The reference I use for skin effect is mostly “Reference Data For Radio Engineers”, a classic reference by Howard W. Sams Inc publications, which is a subsidiary of ITT.
It gives one the tools to figure skin effect at any diameter and for any standard material.
It is more complicated then a single formula, with correction factors for other considerations.

One such consideration is the case of parallel wires. Clearly, if the parallel wires are far away from each other, the interactive forces between electrons in one wire have near zero impact on electrons in the other wire. As a rule, a distance of 10 times the diameter between wires is considered far enough for any interaction. But at a distance of say about 4 times the diameter, the cross influence between conductors carrying current in the same direction is starting to be noticed, and that is an important factor for stranded high frequency wires manufacturers... A lot of thin wires do yield more surface area then one thick solid wire with the same overall diameter, yet the thickness and distance between can be optimized for high frequency. Even a simple wire design can be such a complicated thing… BUT NOT FOR AUDIO FREQUENCIES…  

There are of course many other references with more direct results – already computed For standard copper wire of standard AWG diameters.

As I mentioned, the concept of skin depth is not a “brick wall” divding the copper into conduction and non conduction zones. The current density decreases as we get nearer the wire center, and the skin depth is where the current density is at 37% compared to the value at the surface (37% is 1/e). Now that skin depth concept is based on the assumption that the wire diameter is significantly larger then the skin depth. Skin depth could be misleading to the novice. Skin depth of say 1mm does not mean you can get by with a 1mm or 2mm wire diameter. You need at least 3mm, and 4-5mm diameter is better. Going any further may be a waste of material…

The important concept is RAC/RDC – the ratio between DC resistance and AC resistance at a given frequency. BUT NOT FOR AUDIO FREQUENCIES (where skin effect is negligable)…

The reason people talk about skin effect in audio is a MARKETING one, nothing else!

Regards
Dan Lavry
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David Satz

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Re: Conductance in different materials.
« Reply #16 on: February 10, 2005, 09:52:00 AM »

Dan,

It was great to see/hear you at the New York AES meeting earlier this week. Thank you for coming in and speaking with us.

--Regarding skin effect, the reference numbers for the K factor that you gave three messages back were for a single, solid conductor, no? In stranded wire, skin effect is lessened even further because it really applies to each strand individually. So the use of stranded wire not only helps to prevent breakage when a wire is bent, but it also brings the wire's resistance at high frequencies considerably closer to its DC resistance.

Stranded wire is what nearly everybody uses for audio cables. So if those K numbers were for solid conductors, then in practice, skin effect at audio frequencies matters even less than they would indicate. Maybe that 100-foot "zip cord" speaker wire isn't so bad after all!

--best regards
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danlavry

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Re: Conductance in different materials.
« Reply #17 on: February 11, 2005, 06:30:24 PM »

David Satz wrote on Thu, 10 February 2005 14:52

Dan,

It was great to see/hear you at the New York AES meeting earlier this week. Thank you for coming in and speaking with us.

--Regarding skin effect, the reference numbers for the K factor that you gave three messages back were for a single, solid conductor, no? In stranded wire, skin effect is lessened even further because it really applies to each strand individually. So the use of stranded wire not only helps to prevent breakage when a wire is bent, but it also brings the wire's resistance at high frequencies considerably closer to its DC resistance.

Stranded wire is what nearly everybody uses for audio cables. So if those K numbers were for solid conductors, then in practice, skin effect at audio frequencies matters even less than they would indicate. Maybe that 100-foot "zip cord" speaker wire isn't so bad after all!

--best regards


quote title=David Satz wrote on Thu, 10 February 2005 14:52]Dan,

It was great to see/hear you at the New York AES meeting earlier this week. Thank you for coming in and speaking with us.

--Regarding skin effect, the reference numbers for the K factor that you gave three messages back were for a single, solid conductor, no? In stranded wire, skin effect is lessened even further because it really applies to each strand individually. So the use of stranded wire not only helps to prevent breakage when a wire is bent, but it also brings the wire's resistance at high frequencies considerably closer to its DC resistance.

Stranded wire is what nearly everybody uses for audio cables. So if those K numbers were for solid conductors, then in practice, skin effect at audio frequencies matters even less than they would indicate. Maybe that 100-foot "zip cord" speaker wire isn't so bad after all!

--best regards[/quote]


Hello David,

It was great to be in NY, and I lucked out missing the cold weather.

Yes I was talking about a single solid wire, and the concept of "skin depth" is also for a single wire.
There are at least 2 reasons for the use of stranded wires instead of solid:

The first one is most obvious - mechanical flexibility (such as for the AC chords we use at home to light the lamps, power the TV......) the 60Hz AC application has nothing to do with skin effect.

The second reason is for carrying high frequency signals, way faster then audio.

If we take a circular cross sectional area of a given diameter, and fill it with solid copper, the circumference is well known, and so is the surface of that wire. It is also correct to say that one may fill the same cross sectional area with a tight fit of many smaller diameter wires and the combined surface will be much higher which will reduce the skin effect.

However, it is a common misconception that the skin effect improvement is proportional to the combined surface area packed into the available space. There are 2 reasons why the relationship is not linear:
1. Each wire strand must have enough diameters to take advantage of the "skin depth" concept and in practical terms, each strand must be at least 3-4 times the skin depth, or else the electrons will not "be concentrated on the skin".
2. The resistance of say 10 wire strands is not always one tenth of a single strand because when you "bunch wires together" the electrons on one wire interact with electrons from other wire strands with forces that counteract the multi wire improvement.

So yes, stranded wire has lower skin effect, but a wire design can be optimized electrically for say 10MHz, for 100Mhz, for 1GHz all calling for different dimensions, and there is of course a whole other set of requirements namely mechanical considerations...

Having said all that, skin effect is of no consequence for audio frequencies. It is a marketing hype!

Regards
Dan Lavry
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ammitsboel

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Re: Conductance in different materials.
« Reply #18 on: February 11, 2005, 08:17:19 PM »

Is there a scientific explanation to the sound differences in stranded and solid core cables? let's just say speakers cables.
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bblackwood

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Re: Conductance in different materials.
« Reply #19 on: February 12, 2005, 08:04:31 AM »

ammitsboel wrote on Fri, 11 February 2005 19:17

Is there a scientific explanation to the sound differences in stranded and solid core cables? let's just say speakers cables.

I think you'd first have to show that there was scientific proof of said difference. To my knowledge, no one has ever passed a true double-blind test on similar (low capacitance) cables...
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danlavry

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Re: Conductance in different materials.
« Reply #20 on: February 12, 2005, 08:31:26 PM »

Summary:

The sonic differences one hears, and the electrical differences one measures regarding speaker wires have more to do with the concept of "wire pair" than an individual wire. The characteristics of a wire pair are defined by their relative geometry. A proper test comparing solid to stranded wire calls for identical geometries. Below is the only explanation I can come up with for sonic differences due to reasonable gauge speaker wire:

Details:

I previously stated that speaker wire performance is not influenced by skin effect. In another thread I talked about capacitance, and at very low impedances, capacitance of the cable (especially with short distances such as speaker cables) is not going to alter the signal by any amount you can hear. That leaves resistance and inductance.

Speakers are complicated devices. A good approximation to view a speaker (a driver), often used by speaker designers is an equivalent circuit developed by Thiele and Small, and the equivalent circuit parameters are often available from the driver manufacturers. Note that the parameters consist of both electrical and electromechanical resistances, inductances and capacitance so that the designer ends up with a electrical network describing a speaker driver. Each driver (be it a sub woofer, woofer or tweeter) is far from optimal or desirable device, having an electrical peak (resonance), a mechanical resonance and certainly a need to be corrected (compensated) with a network. The compensation is mostly done via conjugate filters - a circuit made of "real" resistors, capacitors and sometimes inductors to "counteract" the combination of electric and electromechanical behavior of the driver. One such common network is a Zobel Circuit, but there are others... So a speaker cabinet can be looked at as 2-3 drivers with some crossover networks and compensation networks, and one of the goals is to have a constant restive impedance across the audio range (such as 8 Ohms)...

I looked at some of the networks wondering about how much series resistance and inductance it would take to alter the response or ruin the compensation of the drivers or the crossover networks. At first glance it does not seem possible that the resistance of a 10-30 feet of say 12 gauge wire could do much at all. But I would say it is possible to have just enough inductance to interact with the network in a way that will cause a little bit of high frequency loss. I am including a plot for a very simplistic model, assuming a perfect speaker (8 Ohm resistive load over the audio range) and the effect of a cable inductance, assuming 1uH per foot. The picture shows amplitude response to 20KHz for 10feet, 20 feet and 30 feet distance.

Note that we are talking about PASSIVE speakers. All I am saying is NOT true for active (powered speaker), where the whole issue of cable type goes away completely.

Also Note that while resistive variations due to wire are very small to impact the frequency response, a power amplifier output impedance can have an impact.

Below: the red line (10 feet cable) shows around .1dB loss at 20KHz. The Black (30 feet cable) line shows almost a dB at 20Kh and a 1/4dB at 10KHz. It all assumes 1uH per foot and an ideal 8 Ohms speaker. This plot is just a rough first aproximation.  

index.php/fa/667/0/  

I did not answer your question directly regarding solid vs. stranded wire. However, while this answer is indirect, it may hold a key to sonic differences. I assumed (for the graph) 1uH per foot, which is "in the ball park". A reduction would make the response flatter and more inductance would make it worse.

As a rule, a pair of conductors have less inductance when they are closer. Taking 2 individual conductors such as solid copper with thick insulation, and running the "hot" and the "return" far apart yields more inductance than a tightly paralleled pair.

I wonder if the conclusion regarding solid vs stranded resulted from a test where other variables (such as difference in inductance) were unnoticed.

Best Regards
Dan Lavry
www.lavryengineering.com
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