| Place of Origin: | China |
|---|---|
| Brand Name: | Rvyuan |
| Certification: | UL/ISO/SGS |
| Model Number: | Class 180 - 220 |
| Minimum Order Quantity: | 20-100kg |
| Price: | Negotiation |
| Packaging Details: | Carton and pallet |
| Delivery Time: | within 5-10 working days |
| Payment Terms: | L/C, T/T |
| Width-Thickness Ratio: | 1:1.5~1:25 | Conductor Thicknes:: | 0.02-1.8mm |
|---|---|---|---|
| Color: | Copper | Insulation: | UEW/AIW/EIW |
| Thermal Class: | 180/220 | Equivalent Round Wire Diameter:: | 0.12~3.2mm |
| Bonding Method:: | Solvent/hot Wind | ||
| Highlight: | self bonding copper wire,enameled magnet wire |
||
SELF BONDING ULTRA FINE COPPER WIRE CLASEE 180-220 0.02-1.8MM THICKNESS
Self bonding rectangular enamled copper wire is widely usde in wireless charger, our customer including Sumsung's supply, We can provide class 180 to 220 with UEW to AIW insulation with self bonding layer. you can also tell us the thickness of insulation, we will evaluate whether we can make it.
FEATURES AND BENEFITS
The enamelled flat copper wire can form a bigger cross-sectional coil area than an enamelled round copper wire in the same winding space, so the coil can obtain a lower electrical resistance to prevent appliance overheat and more suitable for high-current loading with the current up to 40A above.
The enamelled flat copper wire can form a bigger surface area of the coil than an enamelled round copper wire under the same conductor resistance (meaning the same cross-sectional area), makes it significantly mitigate the skin effect with some high frequency transmission up to 100 KHz.
The enamelled flat copper wire can create a comparative higher space factor, as well as a lower volume-occupation, presenting its advantageous as a lighter, thinner, shorter and smaller product.
APPLICATION
Notebook coil.
Coils of printer.
Motors of CD driver.
Transformer.
Speaker
SPECIFICATION
|
Nominal Diameter mm |
Tolerance |
Min. Increase of Diameter |
Max. Overall Diameter |
Breakdown Voltage |
|
Elongation |
Pin Hole |
Electrical Resistance |
|
|
|
mm |
|
|
≥ V |
|
≥% |
≤Default/5m |
Ω/km (20℃) |
|
|
|
|
|
|
Mandrel Method |
Twisted Method |
|
|
Min. |
Max. |
|
0.012 |
---- |
0.013 |
0.015 |
50 |
---- |
5 |
10 |
142.64 |
157.65 |
|
0.013 |
---- |
0.015 |
0.017 |
70 |
---- |
5 |
10 |
118.41 |
133.98 |
|
0.014 |
---- |
0.016 |
0.018 |
70 |
---- |
5 |
10 |
102.64 |
120.45 |
|
0.015 |
---- |
0.017 |
0.02 |
80 |
---- |
5 |
10 |
89.83 |
104.41 |
|
0.016 |
---- |
0.018 |
0.021 |
90 |
---- |
5 |
8 |
74.67 |
97.56 |
|
0.017 |
---- |
0.019 |
0.022 |
90 |
---- |
5 |
8 |
66.6 |
85.75 |
|
0.018 |
---- |
0.02 |
0.023 |
100 |
---- |
5 |
8 |
59.77 |
75.95 |
|
0.019 |
---- |
0.021 |
0.024 |
100 |
---- |
5 |
8 |
53.95 |
67.75 |
|
0.02 |
0.001 |
0.022 |
0.024 |
100 |
---- |
8 |
8 |
51.83 |
60.81 |
|
0.05 |
±0.002 |
0.007 |
0.062 |
400 |
1200 |
12 |
5 |
7981 |
9528 |
|
0.055 |
±0.002 |
0.007 |
0.068 |
400 |
1200 |
12 |
5 |
6642 |
7815 |
|
0.06 |
±0.002 |
0.007 |
0.073 |
500 |
1200 |
14 |
5 |
5614 |
6526 |
|
0.065 |
±0.002 |
0.007 |
0.078 |
500 |
1200 |
14 |
5 |
4807 |
5531 |
|
0.07 |
±0.002 |
0.007 |
0.083 |
500 |
1200 |
15 |
5 |
4163 |
4747 |
|
0.075 |
±0.002 |
0.007 |
0.088 |
550 |
1200 |
15 |
5 |
3640 |
4119 |
|
0.08 |
±0.002 |
0.008 |
0.094 |
550 |
1200 |
16 |
5 |
3209 |
3608 |
|
0.085 |
±0.002 |
0.008 |
0.099 |
550 |
1200 |
16 |
5 |
2851 |
3187 |
|
0.09 |
±0.002 |
0.01 |
0.106 |
650 |
1200 |
16 |
5 |
2550 |
2835 |
|
0.095 |
±0.002 |
0.01 |
0.111 |
650 |
1200 |
17 |
5 |
2294 |
2538 |
|
0.1 |
±0.002 |
0.011 |
0.118 |
650 |
1200 |
17 |
5 |
2074 |
2286 |
|
0.11 |
±0.002 |
0.011 |
0.129 |
---- |
1300 |
17 |
5 |
1720 |
1882 |
|
0.12 |
±0.002 |
0.011 |
0.139 |
---- |
1500 |
17 |
5 |
1450 |
1577 |
|
0.13 |
±0.002 |
0.011 |
0.149 |
---- |
1500 |
18 |
5 |
1239 |
1340 |
|
0.14 |
±0.002 |
0.011 |
0.159 |
---- |
1600 |
19 |
5 |
1070 |
1153 |
|
0.15 |
±0.002 |
0.011 |
0.169 |
---- |
1700 |
20 |
5 |
934.1 |
1002 |
|
0.16 |
±0.002 |
0.012 |
0.18 |
---- |
1700 |
21 |
5 |
822.3 |
879.4 |
|
0.17 |
±0.003 |
0.013 |
0.192 |
---- |
2000 |
22 |
5 |
721.1 |
787.1 |
|
0.18 |
±0.003 |
0.014 |
0.204 |
---- |
2000 |
22 |
5 |
644.4 |
700.7 |
|
0.19 |
±0.003 |
0.014 |
0.214 |
---- |
2000 |
23 |
5 |
579.4 |
627.8 |
|
0.2 |
±0.003 |
0.014 |
0.224 |
---- |
2000 |
23 |
5 |
523.7 |
565.7 |
