David Brown wrote:
>
>>According to:
>>
>>formatting link
>>
>>stranded wire *does* help reduce skin effect. I think the idea is that
>>although the strands are not insulated from each other directly, there
>>is still a significant resistance between the strands (due to poor
>>contact, air gaps, corrosion, migration of chemicals from the outer
>>insulation, etc.). Thus stranded wire ends up somewhere between solid
>>core and Litz wire regarding skin effect.
>
>Opinions seem about equally divided on this. Anybody know for sure?
See _Stranded Wire With Uninsulated Strands as a Low-Cost Alternative to Litz Wire_ in the References below.
Consider three stranded wires of equal cross section. To simplify the thought experiment, assume square/triangular/hexagonal strands so that there is no space between them.
Wire "Litz" has infinite resistance between strands. Wire "Stranded" has finite resistance between strands. Wire "Solid" has zero resistance between strands.
The basic physics of electromagnetism is such that strands at the center of the bundle experience a greater magnetic flux than strands on the outside. This increases the self-induction-caused back EMF for the center strands, which causes the current to want to jump strands to concentrate at the outer, lower Z strands. "Solid" has no resistance to hinder this, and thus has maximum skin effect.
Many people are under the false impression that simply insulating the strands will create something that they call "Litz wire" that will avoid the current concentrating on the outside of the bundle. A moment's thought will reveal that this cannot be true. Nothing about insulating the strands changes the fact that the center strands have a higher impedance, or that in a parallel circuit the lower-impedance path has more current going through it. They are confusing insulated-strand wire with Litzendraht wire -- the word "Litzendraht" meaning "Woven." In Litzendraht wire, the strands are insulated and then woven so that they take turns being on the outside. There are also related effects that complicate things such as proximity effect and AC current jumping between insulated strands through capacitive coupling.
Now consider wire "Stranded." The resistance between the strands is not infinite (maximum voltage, zero current, zero power dissipated) like wire "Litz" nor is it zero (maximum current, zero voltage, zero power dissipated) like wire "Solid." Instead it has a resistance that reflects the copper oxide layer and the series of point contacts. This keeps some of the current from jumping strands and makes the wire act like something between the "Solid" and "Litz" cases -- and this resistance varies over time, temperature, cable flexing, and perhaps phase of the moon. It also dissipates power, but this appears to be something the RF fellows worry about, not us AC power folks.
That being said, when dealing with 60 Hz. AC power and high current (thick) conductors, you can pretty much ignore all of that and assume that the stranded wire will not have enough skin effect to reduce the capacity of the wire. And, of course, in speaker wire applications the wires are not thick enough to have any noticeable effect -- especially considering the response curves of all available tweeters.
Another helpful hint is that wire with a few large strands tends to keep the same strand in the center, while wire with many fine strands tends to weave them in and out. Consider a long run where partway down the run the current has mostly migrated to the outside. if that outside conductor dives into the center, it will take the current with it, and the current has to migrate all over again.
References:
_Stranded Wire With Uninsulated Strands as a Low-Cost Alternative to Litz Wire_
_Litz wire Applications_ [
_Optimal Choice for Number of Strands in a Litz-Wire Transformer Winding_ [
_Cost-Constrained Selection of Strand Wire and Number in a Litz-Wire Transformer Winding_ [
_Computationally Efficient Winding Loss Calculation with Multiple Windings, Arbitrary Waveforms, and Two- or Three- Dimensional Field Geometry_ [
_Scots Guide: Skin Effect and cable impedance_
_Dartmouth Magnetic Component and Power Electronics Research Transformers and Inductors for Electronics Applications_