Nanocrystalline Toroidal Core For High Frequency Induction Heating Power
● Inverter Welding machine power supply
● X-ray, laser, communication power supply
● UPS and high frequency induction heating power supply
● Frequency control of motor speed power supply
● Charging power supply
● UPS
● High Bs - Reducing volume and weight of the cores
● High permeability and low Coercive force --Higher efficiency and less excited power of transformer
● Low Br (Br≤0.2T) - Higher magnetic flux density and output power
● Low core loss - Lower temperature rising,higher efficiency of the transformer
● Keep stable working at -45℃ ~ 130 ℃ for long time.
| Item | Performance |
| Material Composition | FeCuNbSiB |
| Thickness（um） | 28~35 |
| Saturation induction Bs (T) | 1.25 |
| Curie temperature(oC) | 570oC |
| Hardness Hv | 880 |
| Crystalline temperature Tc(oC) | 500oC |
| Saturation magnetostriction | 2×10-6 |
| Initial permeability μi | ≥80000 |
| Maximum permeability um | ≥500000 |
| Density（g/cm³ ） | 7.2 |
| electrical resistivity(μΩ.cm) | 130 |
| Lamination factor | ≥0.8 |
| Operating Temperature Range | -50~120℃ |
| Code No | Core size(mm) | Case size(mm) | AC(cm2) | Le(cm) | Weight(g) | Suitable Power | ||||
| OD | ID | HT | OD | ID | HT | Ac | Lm | W | kW | |
| JJ-5020 | 50 | 32 | 20 | 54 | 28 | 24 | 1.35 | 12.87 | 125 | 1-1.5 |
| JJ-6420 | 64 | 40 | 20 | 66 | 37 | 23 | 1.72 | 16.30 | 215 | 1-2 |
| JJ-7020 | 70 | 40 | 20 | 75 | 36 | 25 | 2.03 | 17.28 | 265 | 1-2 |
| JJ-7025 | 70 | 40 | 25 | 72 | 37 | 28 | 2.81 | 17.30 | 352 | 3 |
| JJ-8025 | 80 | 50 | 25 | 85 | 44 | 30 | 2.81 | 20.40 | 416 | 3 |
| JJ-10025 | 100 | 50 | 25 | 105 | 45 | 44 | 4.69 | 23.56 | 805 | 8 |
| PTC-10020 | 100 | 60 | 20 | 105 | 56 | 23 | 2.88 | 25.10 | 540 | 3-4 |
| JJ-10530 | 105 | 60 | 30 | 110 | 57 | 35 | 5.00 | 25.90 | 957 | 8-10 |
| JJ-10540 | 105 | 60 | 40 | 110 | 57 | 34 | 6.30 | 26.06 | 1267 | 10-15 |
| JJ-11020 | 110 | 60 | 20 | 116 | 55 | 25 | 3.50 | 26.69 | 725 | 5-7 |
| JJ-11025 | 110 | 60 | 25 | 115 | 54 | 30 | 4.37 | 26.69 | 907 | 6-9 |
| JJ-11030 | 110 | 60 | 30 | 115 | 55 | 35 | 5.25 | 26.69 | 1081 | 8-10 |
| JJ-12030 | 120 | 60 | 30 | 125 | 57 | 35 | 6.48 | 28.20 | 1384 | 12-15 |
| JJ-12020 | 120 | 70 | 20 | 125 | 67 | 25 | 3.60 | 29.80 | 811 | 10 |
| JJ-12025 | 120 | 70 | 25 | 125 | 67 | 30 | 4.60 | 29.80 | 1014 | 8-10 |
| JJ-12030 | 120 | 70 | 30 | 125 | 67 | 35 | 5.40 | 29.80 | 1217 | 10-12 |
| JJ-12040 | 120 | 70 | 40 | 125 | 67 | 47 | 7.50 | 29.80 | 1538 | 12-18 |
| JJ-13040 | 130 | 80 | 40 | 136 | 76 | 45 | 7.20 | 30.30 | 1793 | 15-20 |
| JJ-13050 | 130 | 80 | 50 | 136 | 76 | 55 | 9.00 | 32.90 | 2242 | 20-25 |
| JJ-13050 | 130 | 90 | 50 | 136 | 85 | 56 | 7.50 | 34.50 | 1879 | 20-25 |
| JJ-8020 | 80 | 50 | 20 | 85 | 44 | 25 | 2.10 | 20.56 | 332 | 2-3 |
| JJ-13060 | 130 | 80 | 60 | 136 | 76 | 66 | 11.25 | 32.99 | 2700 | 22-28 |
TAG: nanocrystalline transformer core,nanocrystalline core material,nanocrystalline ribbon
|
P12 JoinChina |
VAC |
core dimensions |
Iron cross section |
Mean path length |
Weight |
permeability(μat 10KHz) |
AL Nominal |
Saturation current typical/A |
||||
|
OD*ID*H |
OD*ID*H |
|||||||||||
|
cm2 |
cm |
g |
Specified value |
Design refer |
10KHz |
100KHz |
10KHz |
100KHz |
||||
|
JJ-1005-W01 |
W914 |
9.8*6.5*4.5 |
11.2*5.1*5.8 |
0.06 |
2.6 |
1.1 |
65600≤μ≤127000 |
87000 |
25.5 |
6.4 |
0.2 |
0.4 |
|
JJ-1205-W01 |
W902 |
12*8*4.5 |
14.1*6.6*6.3 |
0.07 |
3.1 |
1.7 |
72000≤μ≤139000 |
97000 |
28 |
6.8 |
0.2 |
0.4 |
|
JJ-1305-W01 |
W498 |
12.5*10*5 |
14.3*8.5*7.0 |
0.05 |
3.5 |
1.3 |
42200≤μ≤81500 |
56000 |
10 |
3.6 |
0.4 |
0.8 |
|
JJ-1505-W01 |
W865 |
15*10*4.5 |
17.1*7.9*6.5 |
0.09 |
3.9 |
2.6 |
72000≤μ≤139000 |
94000 |
27 |
6.7 |
0.3 |
0.5 |
|
JJ-1606-W01 |
W403 |
16*10*6 |
17.9*8.1*8.1 |
0.14 |
4.1 |
4 |
72000≤μ≤135000 |
97000 |
43 |
10.1 |
0.3 |
0.6 |
|
JJ-1606-W02 |
W308 |
4 |
18000≤μ≤35000 |
23700 |
11.7 |
6.5 |
1.2 |
1.7 |
||||
|
JJ-1806-W01 |
W515 |
17.5*12.6*6 |
19.0*11.0*8.0 |
0.12 |
4.7 |
4.1 |
72000≤μ≤135000 |
96000 |
30 |
6.9 |
0.3 |
0.7 |
|
JJ-1910-W01 |
W838 |
19*15*10 |
21.2*13.0*12.3 |
0.16 |
5.3 |
6.3 |
72000≤μ≤130000 |
96000 |
36.1 |
8.8 |
0.4 |
0.7 |
|
JJ-2008-W01 |
W409 |
20*12.5*8 |
22.6*10.3*10.2 |
0.24 |
5.1 |
9 |
72000≤μ≤135000 |
97000 |
55.2 |
13.6 |
0.4 |
0.7 |
|
JJ-2008-W02 |
W450 |
9 |
18100≤μ≤35000 |
23700 |
14.3 |
9.1 |
1.4 |
2.1 |
||||
|
JJ-2510-W01 |
W523 |
25*20*10 |
27.6*17.4*12.8 |
0.20 |
7.1 |
10.4 |
60000≤μ≤116000 |
80000 |
28.4 |
7.3 |
0.6 |
1.1 |
|
JC-2508-W01 |
W380 |
25*16*10 |
27.9*13.6*12.5 |
0.36 |
6.4 |
17 |
72000≤μ≤135000 |
95000 |
65.5 |
15.5 |
0.4 |
0.9 |
|
JJ-2508-W02 |
W451 |
17 |
15000≤μ≤35000 |
24300 |
17 |
11.5 |
1.7 |
2.6 |
||||
|
JJ-2508-W03 |
W980 |
17 |
3300≤μ≤6400(100KHZ) |
4400 |
3.2 |
3.1 |
9.3 |
9.6 |
||||
|
JC-3010-W01 |
W423 |
30*20*10 |
32.8*17.6*12.5 |
0.40 |
7.9 |
23 |
72000≤μ≤135000 |
103000 |
59.3 |
14 |
0.5 |
1 |
|
JJ-3010-W02 |
W358 |
23 |
19500≤μ≤35200 |
25500 |
15.5 |
11.1 |
2.1 |
3.1 |
||||
|
JJ-3010-W03 |
W981 |
23 |
3280≤μ≤6400(100KHZ) |
4400 |
2.9 |
2.8 |
11.4 |
11.8 |
||||
|
JJ-3015-W01 |
W514 |
30*20*15 |
32.8*17.5*17.8 |
0.57 |
7.9 |
33 |
72000≤μ≤135000 |
96000 |
88 |
20 |
0.5 |
1.1 |
|
JJ-4015-W01 |
W422 |
40*32*15 |
43.1*28.7*18.5 |
0.46 |
11.3 |
38 |
72000≤μ≤135000 |
95000 |
47.2 |
11.1 |
0.8 |
1.5 |
|
JJ-4015-W02 |
W452 |
38 |
15000≤μ≤29000 |
20000 |
12.2 |
7.9 |
3.7 |
5.1 |
||||
|
JJ-4015-W03 |
W964 |
38 |
3160≤μ≤6300 (100KHZ) |
4300 |
2.3 |
2.2 |
16.6 |
17.1 |
||||
|
JJ-4015X-B01 |
W424 |
40*25*15 |
43.1*22.5*18.5 |
0.86 |
10.2 |
64 |
72000≤μ≤135000 |
94000 |
101 |
23.1 |
0.7 |
1.4 |
|
JJ-4015X-B02 |
W453 |
64 |
17850≤μ≤34500 |
23700 |
25.4 |
17.2 |
2.9 |
4.2 |
||||
|
JJ-4515-B01 |
V102 |
45*30*15 |
48.3*26.4*18.2 |
0.86 |
11.8 |
74 |
72000≤μ≤135000 |
96000 |
87.5 |
20.3 |
0.8 |
1.6 |
|
JJ-4515-B02 |
V118 |
74 |
20000≤μ≤38700 |
26700 |
24.3 |
15.9 |
3 |
4.5 |
||||
|
JJ-4515-B03 |
V101 |
74 |
12900≤μ≤25000 |
17200 |
15.7 |
14.3 |
4.6 |
5.8 |
||||
|
JJ-5020-W01 |
W516 |
50*40*20 |
53.5*36.3*23.4 |
0.76 |
14.1 |
79 |
50000≤μ≤97000 |
66000 |
45.3 |
14 |
1.4 |
2.7 |
|
JJ-5020-W02 |
W565 |
79 |
20000≤μ≤38700 |
26600 |
18 |
10 |
3.5 |
5.3 |
||||
|
JJ-6325-B01 |
W517 |
63*50*25 |
67.3*46.5*28.6 |
1.24 |
17.8 |
161 |
50000≤μ≤97000 |
67000 |
58.6 |
18.1 |
1.8 |
3.5 |
|
JJ-6325-B02 |
V110 |
161 |
20000≤μ≤38700 |
26500 |
23.3 |
13.5 |
4.4 |
6.7 |
||||
|
JJ-6325-B03 |
W985 |
163 |
2850≤μ≤5510(100KHZ) |
3700 |
3.3 |
3.2 |
30.2 |
30.9 |
||||
|
JJ-8020-B01 |
V140 |
80*50*20 |
86.0*44.7*25.7 |
2.28 |
20.4 |
342 |
71250≤μ≤137000 |
95000 |
94 |
28 |
1.4 |
2.8 |
|
JC-8020-B02 |
W531 |
342 |
18700≤μ≤36300 ( |
24900 |
35 |
24 |
5.5 |
8.2 |
||||
|
JJ-8020-B03 |
V091 |
347 |
≥5170 |
5170 |
9.6 |
9.2 |
26.4 |
27.3 |
||||
|
JJ-9020-B01 |
W518 |
90*60*20 |
95.4*54.7*24.7 |
2.28 |
23.6 |
395 |
50000≤μ≤97000 |
67000 |
81 |
25.1 |
2.4 |
4.5 |
|
JJ-9020-B02 |
W984 |
400 |
2800≤μ≤5400(100KHZ) |
3700 |
4.6 |
4.5 |
40.9 |
41.8 |
||||
|
JJ-10025-B01 |
V082 |
100*80*25 |
105.5*75.0*29.6 |
1.90 |
28.3 |
379 |
50000≤μ≤97000 |
67000 |
56.3 |
16.9 |
2.8 |
5.3 |
|
JJ-10025-B02 |
V081 |
379 |
12900≤μ≤25000 |
17200 |
14.5 |
13.1 |
10.9 |
13.8 |
||||
|
JJ-10225-B01 |
W468 |
102*76*25 |
108.1*70.0*30.3 |
2.47 |
28.0 |
508 |
50000≤μ≤97000 |
67000 |
68.8 |
21.6 |
3.8 |
6.7 |
|
JJ-10225-B02 |
V080 |
508 |
12900≤μ≤25000 |
17200 |
19.1 |
17.2 |
10.7 |
13.6 |
||||
|
JJ-10225-B03 |
W947 |
515 |
2840≤μ≤5480(100KHZ) |
3800 |
4.3 |
4.2 |
47.7 |
48.5 |
||||
|
JJ-16025-R01 |
V074 |
160*130*25 |
166.9*123.9*30.5 |
2.74 |
45.60 |
917 |
27680≤μ≤59590 |
36000 |
26.8 |
13.7 |
8.4 |
13.6 |
|
JJ-16025-R02 |
V088 |
917 |
20000≤μ≤38700 |
26500 |
20.1 |
13.1 |
11.3 |
17.1 |
||||
|
JJ-16025-R03 |
V066 |
917 |
12900≤μ≤25000 |
17200 |
12.9 |
11.7 |
17.6 |
22.3 |
||||
|
JJ-16025-R04 |
W982 |
967 |
2800≤μ≤5400(100KHZ) |
3700 |
2.9 |
2.9 |
79.3 |
81.1 |
||||
Note: the standard deviation of inductance is (-25% ~+ 45%).
TAG: nanocrystalline transformer core,nanocrystalline core material,nanocrystalline ribbon