HIGH FREQUENCY ENAMELED COPPER LITZ WIRE ROUND 24-44 GAUGE ENAMELED COPPER WIRE
It is constructed of individually insulated magnet wires either twisted or braided into a uniform pattern, as shown in Fig. 1. The twisting pattern is designed to equalize the duration each individual strand of wire spends on the outside of the conductor. Unlike in the simple twisted-strand hookup wire case, the insulations on individual strands force current to be carried equally and evenly along the whole conductor. This reduces the skin effect loss in the conductor, allowing the wires to be used at high frequency up to about 1 MHz
FEATURES
a) Minimize the power losses due to "skin effect".
b) Superior "Q" characteristics at high frequencies.
c) Lower eddy current loss to obtain less equivalent resistance which is advantageous for high voltage and high impedance coils design.
APPLICATION
Width coil, Induction cooker coil, High frequency coil
SPECIFICATION
Gauge(mm) | Stranding No. | Twisting Distance(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 |