EI / AIWJ 220 Grade 1.1mm*0.9mm Rectangular Enameled Copper Wire Flat Winding Wire
EI/AIWJ 220 Grade 1.1mm*0.9mm Rectangular Enameled Copper Wire Flat Winding Wire
In electric vehicles, the compact and lightweight nature of enameled flat wires helps improve the overall efficiency and performance of vehicle propulsion systems. Likewise, in HVAC systems, the use of flat wire allows for more efficient and compact motor designs, which improves energy efficiency and reduces operating costs.
In industrial machinery, the high temperature resistance and reliability of enameled flat wire make it suitable for harsh working conditions. In addition, in household appliances such as washing machines and refrigerators, the use of flat wires helps improve the overall performance and service life of the motor, ensuring long-term reliable operation.
| Model | SFT-AIW | Date | |||||||||
| Size(mm): | 0.900 × 1.100 | Lot | |||||||||
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Key word |
EI/AIWJ 220 Grade 1.1mm*0.9mm Rectangular Enameled Copper Wire Flat Winding Wire |
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Item |
conductor dimension |
Unilateral insulation layer thickness |
Overall dimension |
Dielectric breakdown voltage |
Pinhole | Conductor resistance | Elongation | ||||
| Thickness | Width | Thickness | Width | Thickness | Width | ||||||
| Unit | mm | mm | mm | mm | mm | mm | kv | Pcs/m | Ω/km 20℃ | % | |
|
SPEC |
AVE | 0.900 | 1.100 | 0.025 | 0.025 | ||||||
| Max | 0.930 | 1.160 | 0.040 | 0.040 | 0.980 | 1.200 | 1 | 22.600 | |||
| Min | 0.870 | 1.040 | 0.010 | 0.010 | 0.700 | 0 | 30 | ||||
| No. 1 | 0.907 | 1.108 | 0.028 | 0.033 | 0.962 | 1.174 | 1.200 | 18.300 | 44 | ||
| No. 2 | 1.520 | ||||||||||
| No. 3 | 1.030 | ||||||||||
| No. 4 | 1.514 | ||||||||||
| No. 5 | 1.202 | ||||||||||
| Ave | 0.907 | 1.108 | 0.028 | 0.033 | 0.962 | 1.174 | 1.293 | ||||
| No of reading | 1 | 1 | 1 | 1 | 1 | 1 | 5 | ||||
| Min. reading | 0.907 | 1.108 | 0.028 | 0.033 | 0.962 | 1.174 | 1.030 | ||||
| Max. reading | 0.907 | 1.108 | 0.028 | 0.033 | 0.962 | 1.174 | 1.520 | ||||
| Range | 0.000 | 0.000 | 0.000 | 0.000 | 0.000 | 0.000 | 0.490 | ||||
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