0.05 - 0.4mm Self Bonding Magnet Enameled Wire
0.05 - 0.4 MM SELF BONDING MAGNET ENAMELED WIRE
Magnetic wire can convert an electrical current into a magnetic field. Copper is a particularly good electricity conductor and has little resistance. This keeps electrical currents strong as they pass through each winding of a copper coil, ultimately producing a strong magnetic field. Copper-based magnetic wire is also much smaller than aluminum-based magnetic wire and can fit into smaller areas. Likewise, copper-based magnetic wire can be bent around corners or jointed to provide maximum efficiency.
FEATURE AND BENEFITS
-
Thinning of wire caused by coper melting into molten solder is to minimized. More effective for extra-fine wires.
-
Excellent wettability similar to copper wires.
-
Tensile stength is 5 to 10 percent higher than copper wires.
-
Conductivity 98 percent or more.(IACS)
-
Identical to copper wires in properties of insulating and bonding films.
APPLICATION

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. |
|||
|
0.05 |
±0.002 |
0.011 |
0.067 |
800 |
---- |
12 |
3 |
7981 |
9528 |
|
0.055 |
±0.002 |
0.011 |
0.073 |
800 |
---- |
12 |
3 |
6642 |
7815 |
|
0.06 |
±0.002 |
0.013 |
0.08 |
1000 |
---- |
14 |
3 |
5614 |
6526 |
|
0.065 |
±0.002 |
0.014 |
0.086 |
1000 |
---- |
14 |
3 |
4807 |
5531 |
|
0.07 |
±0.002 |
0.015 |
0.091 |
1000 |
---- |
15 |
3 |
4163 |
4747 |
|
0.075 |
±0.002 |
0.015 |
0.096 |
1100 |
---- |
15 |
3 |
3640 |
4119 |
|
0.08 |
±0.002 |
0.015 |
0.103 |
1100 |
---- |
16 |
3 |
3209 |
3608 |
|
0.085 |
±0.002 |
0.017 |
0.11 |
1200 |
---- |
16 |
3 |
2851 |
3187 |
|
0.09 |
±0.002 |
0.017 |
0.114 |
1200 |
---- |
16 |
3 |
2550 |
2835 |
|
0.095 |
±0.002 |
0.017 |
0.12 |
1200 |
---- |
17 |
3 |
2294 |
2538 |
|
0.1 |
±0.002 |
0.017 |
0.127 |
1200 |
---- |
17 |
3 |
2074 |
2286 |
|
0.11 |
±0.002 |
0.017 |
0.139 |
---- |
2800 |
17 |
3 |
1720 |
1882 |
|
0.12 |
±0.002 |
0.017 |
0.149 |
---- |
2800 |
17 |
3 |
1450 |
1577 |
|
0.13 |
±0.002 |
0.019 |
0.159 |
---- |
2800 |
18 |
3 |
1239 |
1340 |
|
0.14 |
±0.002 |
0.019 |
0.171 |
---- |
3000 |
19 |
3 |
1070 |
1153 |
|
0.15 |
±0.002 |
0.019 |
0.181 |
---- |
3000 |
20 |
3 |
934.1 |
1002 |
|
0.16 |
±0.002 |
0.021 |
0.191 |
---- |
3000 |
21 |
3 |
822.3 |
879.4 |
|
0.17 |
±0.003 |
0.022 |
0.201 |
---- |
3200 |
22 |
3 |
721.1 |
787.1 |
|
0.18 |
±0.003 |
0.022 |
0.211 |
---- |
3200 |
22 |
3 |
644.4 |
700.7 |
|
0.19 |
±0.003 |
0.022 |
0.221 |
---- |
3200 |
23 |
3 |
579.4 |
627.8 |
|
0.2 |
±0.003 |
0.022 |
0.231 |
---- |
3200 |
23 |
3 |
523.7 |
565.7 |
|
0.21 |
±0.003 |
0.027 |
0.248 |
---- |
3300 |
23 |
3 |
475.7 |
512.3 |
|
0.22 |
±0.003 |
0.027 |
0.258 |
---- |
3300 |
23 |
3 |
434 |
466.2 |
|
0.224 |
±0.003 |
0.027 |
0.262 |
---- |
3300 |
23 |
3 |
418.8 |
449.5 |
|
0.23 |
±0.003 |
0.03 |
0.271 |
---- |
3500 |
24 |
3 |
397.5 |
426 |
|
0.24 |
±0.003 |
0.03 |
0.281 |
---- |
3500 |
24 |
3 |
365.5 |
390.8 |
|
0.25 |
±0.003 |
0.03 |
0.291 |
---- |
3500 |
24 |
3 |
337.1 |
359.8 |
|
0.26 |
±0.004 |
0.031 |
0.303 |
---- |
3600 |
25 |
3 |
309.6 |
335 |
|
0.27 |
±0.004 |
0.031 |
0.313 |
---- |
3600 |
25 |
3 |
287.4 |
310.3 |
|
0.28 |
±0.004 |
0.031 |
0.323 |
---- |
3600 |
25 |
3 |
267.6 |
288.2 |
|
0.29 |
±0.004 |
0.033 |
0.335 |
---- |
3700 |
25 |
3 |
249.7 |
268.4 |
|
0.3 |
±0.004 |
0.033 |
0.345 |
---- |
3700 |
25 |
3 |
233.5 |
250.6 |
|
0.31 |
±0.004 |
0.033 |
0.355 |
---- |
3700 |
25 |
3 |
218.9 |
234.4 |
|
0.315 |
±0.004 |
0.033 |
0.36 |
---- |
3700 |
25 |
3 |
212.1 |
227 |
|
0.32 |
±0.004 |
0.036 |
0.368 |
---- |
4000 |
25 |
3 |
205.6 |
219.8 |
|
0.33 |
±0.004 |
0.036 |
0.378 |
---- |
4000 |
25 |
3 |
193.4 |
206.6 |
|
0.35 |
±0.004 |
0.036 |
0.398 |
---- |
4000 |
26 |
3 |
172.2 |
183.4 |
|
0.355 |
±0.004 |
0.036 |
0.403 |
---- |
4000 |
26 |
3 |
167.4 |
178.2 |
|
0.37 |
±0.004 |
0.038 |
0.421 |
---- |
4100 |
26 |
3 |
154.3 |
163.9 |
|
0.38 |
±0.004 |
0.038 |
0.431 |
---- |
4100 |
26 |
3 |
146.4 |
155.3 |
|
0.4 |
±0.004 |
0.038 |
0.451 |
---- |
4100 |
27 |
3 |
132.2 |
140 |
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