Why isn't there a non-conducting core wire for high-frequency coil applicationsDoes solid/multi-stranded/Litz...
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Why isn't there a non-conducting core wire for high-frequency coil applications
Does solid/multi-stranded/Litz wire make a difference in binary serial output?Is the skin effect a factor for low-current AC applications?Would using litz wire for an inductor change the inductance compared to regular wire?Can I build a high-frequency SMPS choke out of an arbitrary coil of wire?Winding my own inductor-resistanceSpaced air core inductor wire size effect?Does stranded wire reduce resistance from skin effect when strands are not insulated?Choosing a wire diameter for an inductorInterleaving in litz wire transformer - to be or not to be?Skin effect with superimposed frequencies
$begingroup$
Background
The commonly known skin effect formulas are derived and only apply to solid conductors. The commonly used "skin depth" only applies in these cases. It is for this reason that in some applications tubes are used, as these are much more weight-efficient than the same diameter wire at a high-enough frequency.
At 1MHz the skin depth of copper wire is 65µm which means that only 40% of the volume of a 1mm diameter wire is carrying 95% of the current, with >35% of it in the outside 20%.
From the skin-depth formulas it is known that a lower conductivity material (e.g., aluminum) has a skin depth that is considerably larger than a higher conductivity one (e.g., copper). As the formula predicts, skin depth is inversely proportional to the square root of the conductivity. If we carry this to its logical consequences, it should be the case that for a conducting tube (which has an insulation core) skin depth should be larger than for an equivalent solid conductor.
As an alternative intuition a thin-walled insulated-core conductor would have nearly twice the surface area of a solid conductor. So it should asymptotically approach nearly half the resistance at a high enough frequency.
In effect, as can be seen in this paper from HB Dwight in 1922 (possible paywall), the increase in resistance w.r.t. frequency for a tube whose wall thickness is 20% of its diameter is more than a factor of two lower than for a solid wire.
From the above curves it can be seen that a tube with t=200µm and d=1mm, due to the increased actual skin depth, should have less than 50% of the impedance increase than a solid d=1mm wire (do note that the curves are normalized w.r.t $ F / R_{dc} $, so interpretation is a bit tricky).
Similar effects (although not as dramatic) can be observed with individually-insulated stranded wire.
Application
In medium-frequency applications, as for example switching power supplies, it is common to use Litz Wire a multi-stranded insulated wire which reduces the losses due to skin effect but becomes less and less effective at higher frequencies (~1MHz) because of the proximity effect and the capacitive coupling of the individual strands.
Probably more gains (particularly with respect to proximity effects) could be obtained if there were multiple individual strands embedded around the periphery of a non-conducting core.
Question
Have I missed something in the theory?
If not, why isn't insulated core wire (either tubes or strands around a core) being commercially exploited for high-frequency inductor applications?
Addendum
As John Birckhead answer points out, flat wire has basically the same advantages with none of the disadvantages (e.g., fill factor). But this leads me to ask:
Why isn't insulated-core flat wire being used for these applications? It should have the same advantage of flat wire with nearly half the resistance at high enough frequencies. Are the possible gains inconsequential?
inductor high-frequency skin-effect litz-wire
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
$endgroup$
add a comment |
$begingroup$
Background
The commonly known skin effect formulas are derived and only apply to solid conductors. The commonly used "skin depth" only applies in these cases. It is for this reason that in some applications tubes are used, as these are much more weight-efficient than the same diameter wire at a high-enough frequency.
At 1MHz the skin depth of copper wire is 65µm which means that only 40% of the volume of a 1mm diameter wire is carrying 95% of the current, with >35% of it in the outside 20%.
From the skin-depth formulas it is known that a lower conductivity material (e.g., aluminum) has a skin depth that is considerably larger than a higher conductivity one (e.g., copper). As the formula predicts, skin depth is inversely proportional to the square root of the conductivity. If we carry this to its logical consequences, it should be the case that for a conducting tube (which has an insulation core) skin depth should be larger than for an equivalent solid conductor.
As an alternative intuition a thin-walled insulated-core conductor would have nearly twice the surface area of a solid conductor. So it should asymptotically approach nearly half the resistance at a high enough frequency.
In effect, as can be seen in this paper from HB Dwight in 1922 (possible paywall), the increase in resistance w.r.t. frequency for a tube whose wall thickness is 20% of its diameter is more than a factor of two lower than for a solid wire.
From the above curves it can be seen that a tube with t=200µm and d=1mm, due to the increased actual skin depth, should have less than 50% of the impedance increase than a solid d=1mm wire (do note that the curves are normalized w.r.t $ F / R_{dc} $, so interpretation is a bit tricky).
Similar effects (although not as dramatic) can be observed with individually-insulated stranded wire.
Application
In medium-frequency applications, as for example switching power supplies, it is common to use Litz Wire a multi-stranded insulated wire which reduces the losses due to skin effect but becomes less and less effective at higher frequencies (~1MHz) because of the proximity effect and the capacitive coupling of the individual strands.
Probably more gains (particularly with respect to proximity effects) could be obtained if there were multiple individual strands embedded around the periphery of a non-conducting core.
Question
Have I missed something in the theory?
If not, why isn't insulated core wire (either tubes or strands around a core) being commercially exploited for high-frequency inductor applications?
Addendum
As John Birckhead answer points out, flat wire has basically the same advantages with none of the disadvantages (e.g., fill factor). But this leads me to ask:
Why isn't insulated-core flat wire being used for these applications? It should have the same advantage of flat wire with nearly half the resistance at high enough frequencies. Are the possible gains inconsequential?
inductor high-frequency skin-effect litz-wire
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
$endgroup$
$begingroup$
Comments are not for extended discussion; this conversation has been moved to chat. Any conclusions reached should be edited back into the question and/or any answer(s).
$endgroup$
– Dave Tweed♦
3 hours ago
$begingroup$
I'll need to read it further, but I found this set of pages on Litz wire. Just a note.
$endgroup$
– jonk
2 hours ago
add a comment |
$begingroup$
Background
The commonly known skin effect formulas are derived and only apply to solid conductors. The commonly used "skin depth" only applies in these cases. It is for this reason that in some applications tubes are used, as these are much more weight-efficient than the same diameter wire at a high-enough frequency.
At 1MHz the skin depth of copper wire is 65µm which means that only 40% of the volume of a 1mm diameter wire is carrying 95% of the current, with >35% of it in the outside 20%.
From the skin-depth formulas it is known that a lower conductivity material (e.g., aluminum) has a skin depth that is considerably larger than a higher conductivity one (e.g., copper). As the formula predicts, skin depth is inversely proportional to the square root of the conductivity. If we carry this to its logical consequences, it should be the case that for a conducting tube (which has an insulation core) skin depth should be larger than for an equivalent solid conductor.
As an alternative intuition a thin-walled insulated-core conductor would have nearly twice the surface area of a solid conductor. So it should asymptotically approach nearly half the resistance at a high enough frequency.
In effect, as can be seen in this paper from HB Dwight in 1922 (possible paywall), the increase in resistance w.r.t. frequency for a tube whose wall thickness is 20% of its diameter is more than a factor of two lower than for a solid wire.
From the above curves it can be seen that a tube with t=200µm and d=1mm, due to the increased actual skin depth, should have less than 50% of the impedance increase than a solid d=1mm wire (do note that the curves are normalized w.r.t $ F / R_{dc} $, so interpretation is a bit tricky).
Similar effects (although not as dramatic) can be observed with individually-insulated stranded wire.
Application
In medium-frequency applications, as for example switching power supplies, it is common to use Litz Wire a multi-stranded insulated wire which reduces the losses due to skin effect but becomes less and less effective at higher frequencies (~1MHz) because of the proximity effect and the capacitive coupling of the individual strands.
Probably more gains (particularly with respect to proximity effects) could be obtained if there were multiple individual strands embedded around the periphery of a non-conducting core.
Question
Have I missed something in the theory?
If not, why isn't insulated core wire (either tubes or strands around a core) being commercially exploited for high-frequency inductor applications?
Addendum
As John Birckhead answer points out, flat wire has basically the same advantages with none of the disadvantages (e.g., fill factor). But this leads me to ask:
Why isn't insulated-core flat wire being used for these applications? It should have the same advantage of flat wire with nearly half the resistance at high enough frequencies. Are the possible gains inconsequential?
inductor high-frequency skin-effect litz-wire
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
$endgroup$
Background
The commonly known skin effect formulas are derived and only apply to solid conductors. The commonly used "skin depth" only applies in these cases. It is for this reason that in some applications tubes are used, as these are much more weight-efficient than the same diameter wire at a high-enough frequency.
At 1MHz the skin depth of copper wire is 65µm which means that only 40% of the volume of a 1mm diameter wire is carrying 95% of the current, with >35% of it in the outside 20%.
From the skin-depth formulas it is known that a lower conductivity material (e.g., aluminum) has a skin depth that is considerably larger than a higher conductivity one (e.g., copper). As the formula predicts, skin depth is inversely proportional to the square root of the conductivity. If we carry this to its logical consequences, it should be the case that for a conducting tube (which has an insulation core) skin depth should be larger than for an equivalent solid conductor.
As an alternative intuition a thin-walled insulated-core conductor would have nearly twice the surface area of a solid conductor. So it should asymptotically approach nearly half the resistance at a high enough frequency.
In effect, as can be seen in this paper from HB Dwight in 1922 (possible paywall), the increase in resistance w.r.t. frequency for a tube whose wall thickness is 20% of its diameter is more than a factor of two lower than for a solid wire.
From the above curves it can be seen that a tube with t=200µm and d=1mm, due to the increased actual skin depth, should have less than 50% of the impedance increase than a solid d=1mm wire (do note that the curves are normalized w.r.t $ F / R_{dc} $, so interpretation is a bit tricky).
Similar effects (although not as dramatic) can be observed with individually-insulated stranded wire.
Application
In medium-frequency applications, as for example switching power supplies, it is common to use Litz Wire a multi-stranded insulated wire which reduces the losses due to skin effect but becomes less and less effective at higher frequencies (~1MHz) because of the proximity effect and the capacitive coupling of the individual strands.
Probably more gains (particularly with respect to proximity effects) could be obtained if there were multiple individual strands embedded around the periphery of a non-conducting core.
Question
Have I missed something in the theory?
If not, why isn't insulated core wire (either tubes or strands around a core) being commercially exploited for high-frequency inductor applications?
Addendum
As John Birckhead answer points out, flat wire has basically the same advantages with none of the disadvantages (e.g., fill factor). But this leads me to ask:
Why isn't insulated-core flat wire being used for these applications? It should have the same advantage of flat wire with nearly half the resistance at high enough frequencies. Are the possible gains inconsequential?
inductor high-frequency skin-effect litz-wire
inductor high-frequency skin-effect litz-wire
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
edited 1 hour ago
Edgar Brown
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
asked 3 hours ago
Edgar BrownEdgar Brown
5,6672731
5,6672731
$begingroup$
Comments are not for extended discussion; this conversation has been moved to chat. Any conclusions reached should be edited back into the question and/or any answer(s).
$endgroup$
– Dave Tweed♦
3 hours ago
$begingroup$
I'll need to read it further, but I found this set of pages on Litz wire. Just a note.
$endgroup$
– jonk
2 hours ago
add a comment |
$begingroup$
Comments are not for extended discussion; this conversation has been moved to chat. Any conclusions reached should be edited back into the question and/or any answer(s).
$endgroup$
– Dave Tweed♦
3 hours ago
$begingroup$
I'll need to read it further, but I found this set of pages on Litz wire. Just a note.
$endgroup$
– jonk
2 hours ago
$begingroup$
Comments are not for extended discussion; this conversation has been moved to chat. Any conclusions reached should be edited back into the question and/or any answer(s).
$endgroup$
– Dave Tweed♦
3 hours ago
$begingroup$
Comments are not for extended discussion; this conversation has been moved to chat. Any conclusions reached should be edited back into the question and/or any answer(s).
$endgroup$
– Dave Tweed♦
3 hours ago
$begingroup$
I'll need to read it further, but I found this set of pages on Litz wire. Just a note.
$endgroup$
– jonk
2 hours ago
$begingroup$
I'll need to read it further, but I found this set of pages on Litz wire. Just a note.
$endgroup$
– jonk
2 hours ago
add a comment |
3 Answers
3
active
oldest
votes
$begingroup$
No, you are correct in the theory, but your approach leads to an unnecessary increase in volume when compared to using flat wire, which is both easier to manufacture and provides a similar advantage for skin effect and the advantage of volumetric efficiency.
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
$endgroup$
1
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
1
$begingroup$
See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
$endgroup$
– Edgar Brown
1 hour ago
2
$begingroup$
First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
$endgroup$
– John Birckhead
1 hour ago
|
show 2 more comments
$begingroup$
Induction Heating (Industrial) commonly uses hollow copper tubing for the inductor.
When you are running 1000 kW or higher, you better believe the copper loss needs to be minimized.
Additionally, the hollow core is used for water cooling.
Sometimes the copper is called "hollow bar". It comes in rectangular or round. It is not uncommon to order a "mill run" to get the hollow bar and thickness desired.
answered 12 mins ago
MarlaMarla
3,89311226
$endgroup$
add a comment |
$begingroup$
There is indeed a variant on insulated core wire for very high frequency applications. It's called a waveguide. It's a hollow tube used for conducting RF. I am of the understanding that the signal travels in the inside of the conducting shell rather than the outside, but the idea of only needing the conducting shell as thick as the skin effect dictates is there.
Not much use for inductors though.
answered 1 hour ago
elchambroelchambro
1112
$endgroup$
add a comment |
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3 Answers
3
active
oldest
votes
3 Answers
3
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
No, you are correct in the theory, but your approach leads to an unnecessary increase in volume when compared to using flat wire, which is both easier to manufacture and provides a similar advantage for skin effect and the advantage of volumetric efficiency.
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
$endgroup$
1
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
1
$begingroup$
See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
$endgroup$
– Edgar Brown
1 hour ago
2
$begingroup$
First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
$endgroup$
– John Birckhead
1 hour ago
|
show 2 more comments
$begingroup$
No, you are correct in the theory, but your approach leads to an unnecessary increase in volume when compared to using flat wire, which is both easier to manufacture and provides a similar advantage for skin effect and the advantage of volumetric efficiency.
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
$endgroup$
1
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
1
$begingroup$
See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
$endgroup$
– Edgar Brown
1 hour ago
2
$begingroup$
First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
$endgroup$
– John Birckhead
1 hour ago
|
show 2 more comments
$begingroup$
No, you are correct in the theory, but your approach leads to an unnecessary increase in volume when compared to using flat wire, which is both easier to manufacture and provides a similar advantage for skin effect and the advantage of volumetric efficiency.
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
$endgroup$
No, you are correct in the theory, but your approach leads to an unnecessary increase in volume when compared to using flat wire, which is both easier to manufacture and provides a similar advantage for skin effect and the advantage of volumetric efficiency.
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
answered 3 hours ago
John BirckheadJohn Birckhead
4,751416
4,751416
1
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
1
$begingroup$
See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
$endgroup$
– Edgar Brown
1 hour ago
2
$begingroup$
First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
$endgroup$
– John Birckhead
1 hour ago
|
show 2 more comments
1
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
1
$begingroup$
See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
$endgroup$
– John Birckhead
2 hours ago
$begingroup$
If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
$endgroup$
– Edgar Brown
1 hour ago
2
$begingroup$
First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
$endgroup$
– John Birckhead
1 hour ago
1
1
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
$begingroup$
I have never seen flat wire being used in RF applications, transformers, or inductors while Litz wire is quite common. Could you expand your answer to point to those and how it compares?
$endgroup$
– Edgar Brown
3 hours ago
1
1
$begingroup$
See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
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– John Birckhead
2 hours ago
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See mouser.com/pdfdocs/bourns_ic046_flatwire_inductor_appnote.pdf
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– John Birckhead
2 hours ago
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To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
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– John Birckhead
2 hours ago
$begingroup$
To your question, Litz wire also has poor volumetric efficiency for high-current applications because of the insulation and the way the wires cross each other in the coil. It is also difficult to terminate at high currents to get an even current distribution. It is useful at low currents when you are not space constrained, because flat wire is tricky to wind.
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– John Birckhead
2 hours ago
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If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
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– Edgar Brown
1 hour ago
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If my intuition is correct, a flat wire with a non-conductive core would have less impedance at higher frequencies than a flat wire (and it should be relatively easy to construct by flattening a thin insulation-filled tube). So, although this points in the right direction and does answer the main aspect of the question, it does not fully address it. Are the gains insignificant, or the application space non-existent?
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– Edgar Brown
1 hour ago
2
2
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First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
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– John Birckhead
1 hour ago
$begingroup$
First of all, thanks for a really interesting and well-stated question, (near to my heart being a magnetics guy). It's just easier flattening the wire down to the skin depth - there would only be a marginal difference because there is insulation between two layers just as there would be insulation in your scenario in the center of the proposed conductor, and you can get the same cross section with a wider flat wire. It would be an interesting study to determine how much if any advantage is gained - it does "feel" like inter-winding capacitance might be less.
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– John Birckhead
1 hour ago
|
show 2 more comments
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Induction Heating (Industrial) commonly uses hollow copper tubing for the inductor.
When you are running 1000 kW or higher, you better believe the copper loss needs to be minimized.
Additionally, the hollow core is used for water cooling.
Sometimes the copper is called "hollow bar". It comes in rectangular or round. It is not uncommon to order a "mill run" to get the hollow bar and thickness desired.
answered 12 mins ago
MarlaMarla
3,89311226
$endgroup$
add a comment |
$begingroup$
Induction Heating (Industrial) commonly uses hollow copper tubing for the inductor.
When you are running 1000 kW or higher, you better believe the copper loss needs to be minimized.
Additionally, the hollow core is used for water cooling.
Sometimes the copper is called "hollow bar". It comes in rectangular or round. It is not uncommon to order a "mill run" to get the hollow bar and thickness desired.
answered 12 mins ago
MarlaMarla
3,89311226
$endgroup$
add a comment |
$begingroup$
Induction Heating (Industrial) commonly uses hollow copper tubing for the inductor.
When you are running 1000 kW or higher, you better believe the copper loss needs to be minimized.
Additionally, the hollow core is used for water cooling.
Sometimes the copper is called "hollow bar". It comes in rectangular or round. It is not uncommon to order a "mill run" to get the hollow bar and thickness desired.
answered 12 mins ago
MarlaMarla
3,89311226
$endgroup$
Induction Heating (Industrial) commonly uses hollow copper tubing for the inductor.
When you are running 1000 kW or higher, you better believe the copper loss needs to be minimized.
Additionally, the hollow core is used for water cooling.
Sometimes the copper is called "hollow bar". It comes in rectangular or round. It is not uncommon to order a "mill run" to get the hollow bar and thickness desired.
answered 12 mins ago
MarlaMarla
3,89311226
answered 12 mins ago
MarlaMarla
3,89311226
answered 12 mins ago
MarlaMarla
3,89311226
answered 12 mins ago
MarlaMarla
3,89311226
3,89311226
add a comment |
add a comment |
$begingroup$
There is indeed a variant on insulated core wire for very high frequency applications. It's called a waveguide. It's a hollow tube used for conducting RF. I am of the understanding that the signal travels in the inside of the conducting shell rather than the outside, but the idea of only needing the conducting shell as thick as the skin effect dictates is there.
Not much use for inductors though.
answered 1 hour ago
elchambroelchambro
1112
$endgroup$
add a comment |
$begingroup$
There is indeed a variant on insulated core wire for very high frequency applications. It's called a waveguide. It's a hollow tube used for conducting RF. I am of the understanding that the signal travels in the inside of the conducting shell rather than the outside, but the idea of only needing the conducting shell as thick as the skin effect dictates is there.
Not much use for inductors though.
answered 1 hour ago
elchambroelchambro
1112
$endgroup$
add a comment |
$begingroup$
There is indeed a variant on insulated core wire for very high frequency applications. It's called a waveguide. It's a hollow tube used for conducting RF. I am of the understanding that the signal travels in the inside of the conducting shell rather than the outside, but the idea of only needing the conducting shell as thick as the skin effect dictates is there.
Not much use for inductors though.
answered 1 hour ago
elchambroelchambro
1112
$endgroup$
There is indeed a variant on insulated core wire for very high frequency applications. It's called a waveguide. It's a hollow tube used for conducting RF. I am of the understanding that the signal travels in the inside of the conducting shell rather than the outside, but the idea of only needing the conducting shell as thick as the skin effect dictates is there.
Not much use for inductors though.
answered 1 hour ago
elchambroelchambro
1112
answered 1 hour ago
elchambroelchambro
1112
answered 1 hour ago
elchambroelchambro
1112
answered 1 hour ago
elchambroelchambro
1112
1112
add a comment |
add a comment |
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Comments are not for extended discussion; this conversation has been moved to chat. Any conclusions reached should be edited back into the question and/or any answer(s).
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– Dave Tweed♦
3 hours ago
$begingroup$
I'll need to read it further, but I found this set of pages on Litz wire. Just a note.
$endgroup$
– jonk
2 hours ago