High Conductivity Enamelled Copper Wire Self Bonding Wire USDC USTC High Frequency Litz Wire
HIGH CONDUCTIVITY ENAMELED COPPER WIRE SELF BONDING WIRE USDC USTC HIGH FREQUENCY LITZ WIRE
Litz wire is constructed of individually insulated magnet wires bunched or braided together in a uniform pattern so that each strand takes all possible positions in the cross section of the overall conductor.The primary benefit of Litz wire is in reducing AC losses in high frequency windings due to the “skin effect”. Current in a solid conductor is concentrated at the periphery. As frequency rises, the current migrates to the skin. The multiple strand construction of Litz allows current to divide uniformly between strands. The AC to DC resistance ratio then tends to equalize which is desirable in high Q circuit applications.
FEATURE
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High conductivity
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Shock resistance
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Excellent durability
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Superior strength
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Rust resistant
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Low maintenance
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Affordability
APPLICATION
Transformer, motor, generator, audio coil, household application, instruments and meters, welding machine etc..
|
Gauge(mm) |
Stranding No. |
e(mm) |
|
0.05+250D |
14 |
2.75 |
|
0. 06+250D |
14-18 |
2.64 |
|
0.06 + 250D |
10 |
3.5 |
|
0.07 + 250D |
36 |
5.3 |
|
0.08+200D |
8 |
2.64 |
|
0.08+250D |
8 |
2.9 |
|
0.08+500D |
10 |
3.5 |
|
0.10-0.14 |
10 or below |
5.68-9.18 |
|
0.10-0.14 |
10-20 |
9.18-11.47 |
|
0.11-0.14 |
30-60 |
15.29-17.00 |
|
0.15-0.20 |
10 or below |
9.18-11.47 |
|
0.15-0.20 |
10-20 |
15.29-17.00 |
|
0.21-0.30 |
10 or below |
11.47-15.29 |
|
0.21-0.30 |
10-20 |
15.29-17.00 |
|
0.31-0.40 |
10 or below |
17.00-22.20 |
|
0.31-0.40 |
10-20 |
22.20-31.57 |
|
0.50 or above |
|
5.68-50.00 |
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