|
Hysteresis loop is approximately rectangular. high saturation flux
density, Bs,ligh remanence, Br, high Cure temperature Tc, lower
coercive force Hc.
|
Saturation(mT): 400㊣5%
Remanence(mT):290㊣5%
Coercive Force(A/m): ≒70
Initial Permeability: 300㊣25% (1KHz)
Specific Resistivity(次. 收): 10^6
Curie Temp(⊥): ˇ250
Specific Weight(g/cm^3): 5.08‵5.2
|
 |
 
|
|
|
米Qfˇ10GHz under the conditions of high-flux(30mT) and high frequency(2-5MHz)
Initial Permeability 米iㄩ800㊣20%
Increment Permeability 米→ㄩ600(when 0 A/m)
Saturation flux density Bsㄩ270mT(25∼C, 800A/m)
﹛﹛﹛﹛﹛﹛﹛﹛﹛﹛Bsㄩ230mT(40∼C, 800A/m)
Coercive force Hcㄩ80A/m(after 800A/m driven)
DC Volume Resistivity 老dcㄩˇ10^7
次﹞cm
Curie Temperature Tcㄩ≡150∼C
|
| |
5mT |
10mT |
20mT |
30mT |
| 1 |
|
|
|
|
| 2 |
|
|
|
|
| 3 |
|
|
|
|
| 4 |
|
|
|
|
| 5 |
|
|
|
|
| 10 |
|
|
|
|
| |
| :::VERY
HIGH FREQUENCY::: |
米i of this serial material is between 50〞800. The material has lower loss
factor at very high frequency (3-50MHz). Insensitive to temperature.
| |
米i(㊣20%) |
Bs (mT) |
Hc(A/m) |
Tg汛/米i﹞10-6 |
Tc(∼C) |
老dc(次﹞cm) |
| R800 |
800 |
340 |
70 |
45(2MHz) |
150 |
|
| R600 |
600 |
350 |
70 |
50(2MHz) |
180 |
|
| R400 |
400 |
400 |
80 |
80(3MHz) |
200 |
|
| R200 |
200 |
380 |
120 |
80(3MHz) |
220 |
|
| R100 |
100 |
380 |
140 |
100(5MHz) |
250 |
|
| 10 |
50 |
360 |
160 |
100(5MHz) |
300 |
|
| |
| ::HIGH
FREQUENCY&HIGH POWER:: |
High flux density, High Cure temperature, High Q, insensitive to temperature.
| |
米i(㊣20%) |
Q(3MHz) |
Bs(mT) |
Tc(°C) |
老dc(次﹞cm) |
| R300p |
300 |
160 |
400 |
350 |
|
| R200p |
200 |
160 |
390 |
350 |
|
| R150p |
150 |
190 |
380 |
360 |
|
| R100p |
100 |
210 |
360 |
360 |
|
| R50p |
50 |
240 |
350 |
360 |
|
| |
| ::::::::WIDE
BAND:::::::: |
Low loss factor at a very wide frequency band. very high 米Qf value. This
material is suitable for wide band communication use.
| |
米i(㊣20%) |
Tg汛/米i﹞10-6 |
Bs(mT) |
Hc(A/m) |
Tc(°C) |
老dc(次﹞cm) |
| R2000W |
2000 |
≒30ㄗ0.1MHzㄘ |
280 |
15 |
100 |
|
| R1500W |
1500 |
≒50ㄗ0.5MHzㄘ |
320 |
18 |
120 |
|
| R1000W |
1000 |
≒40ㄗ0.5MHzㄘ |
340 |
28 |
150 |
|
| R500W |
500 |
≒80ㄗ1.5MHzㄘ |
350 |
50 |
180 |
|
| R300W |
300 |
≒100ㄗ2MHzㄘ |
350 |
60 |
200 |
|
| R100W |
100 |
≒150ㄗ10MHzㄘ |
350 |
80 |
250 |
|
| R50W |
50 |
≒250ㄗ20MHzㄘ |
350 |
120 |
300 |
|
The cut-off frequency of this material is ultra high. It can be used at
multi-tens MHz to GHZ frequency range.
| |
米i(㊣20%) |
米Q(500MHz) |
Bs(mT) |
Hc(A/m) |
Tc(°C) |
老dc(次﹞cm) |
| R10V |
10 |
300 |
280 |
800 |
380 |
|
| R5V |
5 |
300 |
280 |
900 |
390 |
|
| |
| :::HIGH
SUSCEPTIBILITY::: |
The material has high susceptibility, narrow resonance line (→H) and higher
Cure temperature. It can be used for X-band (5200MHz〞1900MHz) and K-band
(15000MHz〞36000MHz) device construction.
Propertiesㄩ
Saturation susceptibilityㄩ4羽Ms≡0.4 T
Width of Resonance lineㄩ→H≒9600 A/m
Cure Temperatureㄩ Tc≡370°C
Permittivityㄩ ﹛﹛汍＞12
Tangent of the loss angleㄩ≒10-3
Volume Resistivityㄩ﹛老dc≡106
次﹞cm
Specific Weightㄩ ﹛≡5 g/cm3
|
 |
|
|
Polyimide/Kapton