SIFERRIT Materials. Siemens Matsushita Components 33

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1 SIFERRIT Materials Based on IEC 60401, the data specified here are typical data for the material in question, which have been determined principally on the basis of ring cores. The purpose of such characteristic material data is to provide the user with improved means for comparing different materials. There is no direct relationship between characteristic material data and the data measured using other core shapes and/or core sizes made of the same material. In the absence of further agreements with the manufacturer, only those specifications given for the core shape and/or core size in question are binding. Siemens Matsushita Components 33

2 SIFERRIT Materials 1 Material application survey Usage Frequency range Specific application Type Material High Q inductors up to 0,1 MHz N 48 Filters in telephony, Gapped P in resonant circuits 0,2 1,6 MHz M 33 MW IF filters and RM cores, and filters 1, 12 MHz K 1 adjusting cores, TT/PR 6 30 MHz K 12 VHF filters up to 100 MHz U 17 Line attenuation up to 2 MHz M 13 K10 Balun transformers Ring cores, doubleaperture cores Broadband transformers (e.g. antenna transformers for MW, SW, VHF, TV) ISDN transformers, digital data transformers (xdsl), current-compensated interference suppression chokes up to 3 MHz T 46 ISDN transformers T 42 Impedance and matching T38 transformers Ring cores RM, P, ER, EP, ring cores T 37 Current-compensated chokes Ring cores, DE cores T 3 RM, P, ring, DE T 6 P, ring cores, TT/PR, EP up to MHz N 30 Current-compensated chokes Ring cores, N 26 Radio-frequency transformers doubleaperture cores up to 10 MHz M 33 up to 20 MHz K 1 K12 up to 400 MHz U 17 Sensors, ID systems up to 1 MHz N 22 Inductive proximity switches P core halves up to 2 MHz M 33 up to 100 MHz FPC 34 Siemens Matsushita Components

3 SIFERRIT Materials Usage Power transformers, chokes Frequency range Material Specific application 1 to 100 khz N 27 Transformers for flyback converters E, EC, ETD, U, RM, PM N 41 Chokes Pot cores, RM up to 200 khz N 3 Diode splitting transformers E, U, UR N 62 E, U, UR, ETD, N 67 High-voltage transformers ER N 72 Electronic lamp ballast E, ETD devices up to 300 khz N 82 Diode splitting transformers U, UR up to 00 khz N 87 Transformers for forward and push-pull converters 0,3 1 MHz N 49 Transformers for DC/DC 0, 1 MHz N 9 converters, particularly resonance converters Type ETD, EFD, RM, TT/PR, ER, ELP EFD, ER, ELP, RM (low profile) Siemens Matsushita Components 3

4 SIFERRIT Materials 2 Material properties Preferred application Resonant circuit inductors Material U 17 1) K 12 1) K 1 M 33 2) N 48 Base material NiZn NiZn NiZn MnZn MnZn Color code (adjuster) gray yellow violet white Symbol Unit Initial permeability (T = 2 C) Meas. field strength Flux density (near saturation) (f = 10 khz) Coercive field strength (f = 10 khz) Optimum frequency range Relative at f min µ i 10 ± 30 % H B S (2 C) B S (100 C) H c (2 C) H c (100 C) A/m mt mt A/m A/m MHz loss factor at f max 10 6 < 1700 tan δ/µ i 10 6 < ± 2 % < 10 < ± 2 % , 12 < 40 < ± 2 % ,2 1,0 < 12 < ± 2 % ,001 0,1 Hysteresis η B 10 6 /mt < 27 < 4 < 36 < 1,8 < 0,4 material constant Curie temperature T C C > 0 > 40 > 400 > 200 > 170 Relative temperature coefficient α F 10 6 /K at 2 C at 20 C Mean value of α F at 2 C , 2,6 2,7 4,2 0,4 0, 0,7 0, 10 6 /K ,6 0,0 Density kg/m Disaccommodation DF factor at 2 C Resistivity ρ Ωm Core shapes P, Double aperture P, Ring RM, P, Ring, P core half RM, P, RM, P Ring, Double aperture, P core half Other material properties (graphs) see page ) Perminvar ferrite: irreversible variations in quality and permeability may occur in case of strong fields in the core (> 100 A/m). In the case of shape-related dimensions, these dimensions may be exceeded by up to %. 2) For threaded cores µi = 600 ± 20% 36 Siemens Matsushita Components

5 SIFERRIT Materials Material properties (continued) Preferred application Inductors for line attenuation Special type Material K 10 M 13 N 22 Base material NiZn NiZn MnZn Color code (adjuster) red Symbol Unit Initial permeability (T = 2 C) Meas. field strength Flux density (near saturation) (f = 10 khz) Coercive field strength (f = 10 khz) Optimum frequency range Relative at f min µ i 800 ± 2 % H B S (2 C) B S (100 C) H c (2 C) H c (100 C) A/m mt mt A/m A/m MHz ,1 1 loss factor at f max 10 6 < 60 tan δ/µ i 10 6 < ± 2 % ,001 0,1 < < ± 2 % ,001 0,2 < 2 < 20 Hysteresis η B 10 6 /mt < < 4 < 1,4 material constant Curie temperature T C C > 10 > 10 > 14 Relative temperature coefficient α F 10 6 /K at 2 C at 20 C Mean value of α F at 2 C 3,0,0,0 7, 10 6 /K 10,0 3,7 0,9 Density kg/m Disaccommodation DF factor at 2 C Resistivity ρ Ωm Core shapes Ring, Double aperture Ring, Double aperture Ring, P core half, Double aperture Other material properties (graphs) see page Siemens Matsushita Components 37

6 SIFERRIT Materials Material properties (continued) Preferred application Broadband transformers Material N 26 N 30 T 6 T 3 T 37 Base material MnZn MnZn MnZn MnZn MnZn Symbol Unit Initial permeability (T = 2 C) Meas. field strength Flux density (near saturation) (f = 10 khz) Coercive field strength (f = 10 khz) Optimum frequency range Relative at f min µ i 2300 ± 2 % H B S (2 C) B S (100 C) H c (2 C) H c (100 C) A/m mt mt A/m A/m MHz ,001 0,1 loss factor at f max 10 6 < 3,8 tan δ/µ i 10 6 < 2, ± 2 % ± 30 % ± 2 % ± 2 % Hysteresis η B 10 6 /mt < 0,3 < 1,1 < 1,1 < 1,1 < 1,1 material constant Curie temperature T C C > 10 > 130 > 160 > 130 > 130 Relative temperature coefficient α F 10 6 /K at 2 C at 2 C Mean value of α F at 2 C 0 1, 0 1, /K 1,0 0,6 0, 0,8 0,3 Density kg/m Disaccommodation DF 10 6 factor at 2 C Resistivity ρ Ωm 2 0, 0,30 0,2 0,2 Core shapes RM, P, EP Ring, DE RM, P, EP, E, Ring, Double aperture RM, P, ER, Ring RM, P, EP, Ring Other material properties (graphs) see page Siemens Matsushita Components

7 SIFERRIT Materials Material properties (continued) Preferred application Broadband transformers Material T 38 T 42 3) T 46 3) Base material MnZn MnZn MnZn Symbol Unit Initial permeability (T = 2 C) Meas. field strength Flux density (near saturation) (f = 10 khz) Coercive field strength (f = 10 khz) Optimum frequency range Relative at f min µ i ± 30 % H B S (2 C) B S (100 C) H c (2 C) H c (100 C) A/m mt mt A/m A/m MHz loss factor at f max 10 6 tan δ/µ i ± 30 % ± 30 % Hysteresis η B 10 6 /mt < 1,4 < 1,4 < 2,0 material constant Curie temperature T C C > 130 > 130 > 130 Relative temperature coefficient α F 10 6 /K at 2 C at 20 C Mean value of α F at 2 C /K 0,4 0,3 0,6 Density kg/m Disaccommodation DF 10 6 factor at 2 C Resistivity ρ Ωm 0,1 0,1 0,01 Core shapes RM, P, EP, ER, E, Ring RM, EP Other material properties (graphs) see page Ring 3) Material values defined on the basis of small ring cores ( R10) Siemens Matsushita Components 39

8 SIFERRIT Materials Material properties (continued) Preferred application Power transformers Material N 9 N 49 N 3 N 82 4) N 62 Base material MnZn MnZn MnZn MnZn MnZn Symbol Unit Initial permeability (T = 2 C) Flux density (H = 1200 A/m, f = 10 khz) Coercive field strength (f = 10 khz) µ i 80 ± 2 % B S (2 C) B S (100 C) H c (2 C) H c (100 C) mt mt A/m A/m Typical frequency range khz Hysteresis material constant 100 khz, 200 mt, 100 C 300 khz, 100 mt, 100 C 00 khz, 0 mt, 100 C 1 MHz, 0 mt, 100 C 1300 ± 2 % ± 2 % ± 2 % η B 10 6 /mt 1900 ± 2 % Curie temperature T C C > 240 > 240 > 240 > 240 > 240 Mean value of α F 10 6 /K at 20 C Density kg/m Relative core losses 2 khz, 200 mt, 100 C P V mw/g mw/cm mw/g mw/cm 3 mw/g mw/cm 3 mw/g mw/cm 3 mw/g mw/cm Resistivity ρ Ωm Core shapes EFD RM, Ring, EFD, ER ELP 10 2 E, U U, UR ETD, E, U Other material properties (graphs) see page ) Preliminary data 40 Siemens Matsushita Components

9 SIFERRIT Materials Material properties (continued) Preferred application Power transformers Material N 27 N 67 ) N 87 N 72 N 41 Base material MnZn MnZn MnZn MnZn MnZn Symbol Unit Initial permeability (T = 2 C) Flux density (H = 1200 A/m, f = 10 khz) Coercive field strength (f = 10 khz) µ i 2000 ± 2 % B S (2 C) B S (100 C) H c (2 C) H c (100 C) mt mt A/m Typical frequency range khz 2 10 Hysteresis material constant 100 khz, 200 mt, 100 C 300 khz, 100 mt, 100 C 00 khz, 0 mt, 100 C 1 MHz, 0 mt, 100 C 2100 ± 2 % ± 2 % ± 2 % ± 2 % η B 10 6 /mt < 1, < 1,4 < 1,4 < 1,4 Curie temperature T C C > 220 > 220 > 210 > 210 > 220 Mean value of α F 10 6 /K at 20 C Density kg/m Relative core losses 2 khz, 200 mt, 100 C P V mw/g mw/cm mw/g mw/cm 3 mw/g mw/cm 3 mw/g mw/cm 3 mw/g mw/cm Resistivity ρ Ωm Core shapes P, PM, ETD, EC, ER, E, U, Ring RM, P, EP, ETD, ER, EFD, E, U, Ring RM, TT, P, PM, ETD, EFD, E, ER, ELP E, EFD RM, P Other material properties (graphs) see page ) Not for new design Siemens Matsushita Components 41

10 SIFERRIT Materials Material properties (continued) Preferred application Injectionmolded parts Film Material Ferrite Polymer Composite (FPC) Base material C302 C30 C31 Symbol Unit Initial permeability µ i 17 ± 20 % 9 ± 20 % 9 ± 20 % f = 1 MHz Flux density (near saturation) B S (2 C) mt H = 2 ka/m f = 10 khz Remanent induction B r (2 C) mt H = 2 ka/m f = 10 khz Coercive field strength H C (2 C) A/m H = 2 ka/m f = 10 khz Relative loss factor tanδ/µ i f = 1 MHz < 0,0004 f = 100 MHz < 0,03 < 0,00 < 0,00 f = 1 GHz < 0,400 < 0,400 Hysteresis material constant η B 10 3 /mt < 0,2 < 2 < 2 Temperature coefficient α= µ/µ T 1/K < 0,0002 < 10 - < 10 - Density kg/m Resistivity ρ Ωm f = 1 khz f = 10 khz f = 10 MHz Relative permittivity f = 1 khz f = 10 khz f = 10 MHz ε r Maximum operating temperature T max C Dielectric strength kv/mm 1 0,8 Tensile strength 6) σ Z N/mm 2 1, 2, Tearing resistance 6) % 2 2 Compressibility 6) κ N/mm Other material properties (graphs) see page ) T = 23 C and 0 % relative humidity 42 Siemens Matsushita Components

11 SIFERRIT Materials 3 Measuring conditions The following measuring conditions, which correspond largely to IEC 60401, apply for the material properties given in the table: Properties (valid only for ring cores of sizes R 10 to R 36) Measuring conditions Frequency khz Field strength (materialdependent) ka/m Max. flux density mt Temperature C Initial permeability µ i 10 0,2 2 B mt 10 1,2 2; 100 Flux density near to saturation Coercive field strength H cb A/m ka/m 10 1,2 near saturation Relative loss factor tan δ/µ i 0,2 2 Hysteresis material constant η B T 1 10 (µ i 00) 100 (µ i < 00) B 1 B 2 1, 3,0 0,3 1,2 Curie temperature T c C 10 0,2 Relative temperature coefficient 2; 100 α F 10 6 /K 10 0, Density kg/m 3 2 Disaccommodation DF ,2 2; 60 1) factor Resistivity ρ Ωm 2 The following properties are given only for materials for power applications: 2 Power loss P V mw/cm 3 mw/g ) Higher temperature than specified by IEC (40 C) Siemens Matsushita Components 43

12 SIFERRIT Materials 4 Specific material data DC magnetic bias I_ N H_ = I e H_ = DC field strength [A/m] I_ = Direct current [A] N = Number of turns l e = Effective magnetic path length [m] The curves of µ rev =f(h_) allow an approximate calculation of the variation in reversible permeability (µ rev ) and A L value caused by magnetic bias. These curves are of particular interest for cores for transformers and chokes, since magnetic bias should be avoided if possible with inductors requiring high stability (filter inductors etc.). In the case of geometrically similar cores (i.e. in particular the same A min /A e ratio) the effective permeability of the core in question in conjunction with the given curves suffices to determine the reversible permeability to a close approximation. 44 Siemens Matsushita Components

13 SIFERRIT Materials Inductors for Resonant Circuits and Line Attenuation Relative loss factor (measured with ring cores, measuring flux density B 0,2 mt) 10-1 FAL067-1 tan δ µ i Line attenuation Resonant circuit K12 U17 K1-10 M13 K10 N48 M33 N26/N khz f 6 10 Siemens Matsushita Components 4

14 SIFERRIT Materials Broadband Transformers Relative inductance component (measured with ring cores, measuring flux density B 0,2 mt) 10 FAL068-9 µ s T46 T42 T38 T37 T3 T6 N N khz 10 4 f 46 Siemens Matsushita Components

15 SIFERRIT Materials Power Transformers Performance factor (measured with ring cores R29, T = 100 C, P V = 300 kw/m 3 ) 0000 khz. mt FAL080-S 4000 f. Bmax N N N82 N N N27 N62 N67 N For definition of performance factor see page khz 4 f Siemens Matsushita Components 47

16 SIFERRIT Materials Broadband and Filter Applications Standardized hysteresis material constant versus temperature 7 FAL073-A η B, T η B, 2 C 6 4 M33 N26 N48 N30 T6 T3 T37 T _ 40 _ C 140 T 48 Siemens Matsushita Components

17 U 17 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Permeability factor versus temperature (measured with P and RM cores, B 0,2 mt), µ i 10 T ( C) α F (10 6 /K) Mean value Siemens Matsushita Components 49

18 U 17 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 0 Siemens Matsushita Components

19 K 12 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Permeability factor versus temperature (measured with P and RM cores, B 0,2 mt), µ i 26 T ( C) α F (10 6 /K) Mean value Siemens Matsushita Components 1

20 K 12 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 2 Siemens Matsushita Components

21 K 1 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Permeability factor versus temperature (measured with P and RM cores, B 0,2 mt), µ i 80 T ( C) α F (10 6 /K) Mean value Siemens Matsushita Components 3

22 K 1 (f = 10 khz, T = 2 C) (f = 10 khz, T =100 C) 4 Siemens Matsushita Components

23 M 33 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Permeability factor versus temperature (measured with P and RM cores, B 0,2 mt), µ i 70 DC magnetic bias of P and RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) T ( C) α F (10 6 /K) Mean value Siemens Matsushita Components

24 M 33 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 6 Siemens Matsushita Components

25 N 48 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) 10 4 µ, µ 10 3 FAL046-D 3000 µ i µ i FAL047-L tanδ µ i tan δ/ µ i f = 100 khz µ µ khz f C 200 T Permeability factor versus temperature (measured with P and RM cores, B 0,2 mt), µ i 2300 FAL074-I µ i - µ 1i µ i µ 1i Relative loss factor tan δ/µ i (measured with R29 ring cores) 10-4 tanδ µ i FAL048-U 0 0 T T ( C) α F (10 6 /K) ) ) C 70 Mean value T khz f ) With P cores P22 13 and RM cores RM 8 the α F value may deviate by up to 1, /K. Siemens Matsushita Components 7

26 N 48 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 40 FAL FAL00-6 mt B 30 T = 2 C f = 10 khz mt B 30 T = 100 C f = 10 khz B sat = 421 mt B r = 122 mt H c = 2,3 A/m 10 0 B sat = 422 mt B r = 12 mt H c = 2,3 A/m A/m 1400 H A/m 1400 H DC magnetic bias of P and RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) 8 Siemens Matsushita Components

27 K 10 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) 10 3 µ, µ FAL07-R µ i B = 0.2 mt N = 10 FAL076-Z tan δ µ i µ i f = 100 khz µ s µ s tan δ/µ i f = 00 khz khz 10 f C 200 T (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 30 mt 300 B FAL mt 300 B FAL078-G A/m 2000 H A/m 200 H Siemens Matsushita Components 9

28 M 13 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R2 ring cores, B 0,2 mt) (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 60 Siemens Matsushita Components

29 N 22 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative loss factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) Siemens Matsushita Components 61

30 N 26 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i and relative los factor tan δ/µ i versus temperature (measured with R10 ring cores, B 0,2 mt) 10 4 µ, µ 10 3 FAL01-E 3000 µ i µ i FAL02-M tanδ µ i µ µ 1000 tan δ/ µ i f = 100 khz khz f C 200 T Permeability factor versus temperature (measured with R10 ring cores, B 0,2 mt) Relative loss factor (measured with R14 ring cores, B 0,2 mt) µ i - µ 1i µ i µ 1i FAL079-P 10-4 tanδ µ i FAL C 80 T khz f Siemens Matsushita Components

31 N 26 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 40 FAL0-C 40 FAL06-K mt B 30 T = 2 C f = 10 khz mt B 30 T = 100 C f = 10 khz B sat = 386 mt B r = 100 mt H c = 23,3 A/m 10 0 B sat = 38 mt B r = 102 mt H c = 23,4 A/m A/m 1400 H A/m 1400 H DC magnetic bias of P and RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 63

32 N 30 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R10 ring cores, B 0,2 mt) Relative loss factor (measured with R20 ring cores, B 0,2 mt) 64 Siemens Matsushita Components

33 N 30 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 6

34 T 6 Complex permeability (measured with R29 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R29 ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R29 ring cores, B 0,2 mt) Relative loss factor (measured with R29 ring cores, B 0,2 mt) 66 Siemens Matsushita Components

35 T 6 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 67

36 T 3 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R16 ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R16 ring cores, B 0,2 mt) Relative loss factor (measured with R16 ring cores, B 0,2 mt) 68 Siemens Matsushita Components

37 T 3 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 69

38 T 37 Complex permeability (measured with R16 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R22 ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R22 ring cores, B 0,2 mt) Relative loss factor (measured with R16 ring cores, B 0,2 mt) 70 Siemens Matsushita Components

39 T 37 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 71

40 T 38 Complex permeability (measured with R14 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R16 ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R16 ring cores, B 0,2 mt) Relative loss factor (measured with R14 ring cores, B 0,2 mt) 72 Siemens Matsushita Components

41 T 38 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 73

42 T 42 Complex permeability (measured with R9, ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R9, ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R9, ring cores, B 0,2 mt) Relative loss factor (measured with R9, ring cores, B 0,2 mt) 74 Siemens Matsushita Components

43 T 42 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 7

44 T 46 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Variation of initial permeability with temperature (measured with R10 ring cores, B 0,2 mt) Relative loss factor (measured with R10 ring cores, B 0,2 mt) 76 Siemens Matsushita Components

45 T 46 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) Siemens Matsushita Components 77

46 N 9 Complex permeability (measured with R2 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R29 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E cores) 78 Siemens Matsushita Components

47 N 9 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 2 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 100 C) Siemens Matsushita Components 79

48 N 9 Relative core losses versus AC field flux density (measured with R29 ring cores) Relative core losses versus temperature (measured with R29 ring cores) Relative core losses (measured with R29 ring cores) 80 Siemens Matsushita Components

49 N 49 Complex permeability (measured with R17 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R17 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E cores) Siemens Matsushita Components 81

50 N 49 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 2 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 100 C) 82 Siemens Matsushita Components

51 N 49 Relative core losses versus AC field flux density (measured with R17 ring cores) Relative core losses versus temperature (measured with R17 ring cores) Relative core losses (measured with R17 ring cores) Siemens Matsushita Components 83

52 N 3 Complex permeability (measured with R29 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R29 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E and U cores) 84 Siemens Matsushita Components

53 N 3 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P, RM, PM, E and U cores ( B 0,2 mt, f = 10 khz, T = 2 C) DC magnetic bias of P, RM, PM, E and U cores ( B 0,2 mt, f = 10 khz, T = 100 C) Siemens Matsushita Components 8

54 N 3 Relative core losses versus AC field flux density (measured with R17 ring cores) Relative core losses versus temperature (measured with R17 ring cores) Relative core losses (measured with R17 ring cores) 86 Siemens Matsushita Components

55 N 82 Complex permeability (measured with R29 ring cores) Initial permeability µ i versus temperature (measured with R29 ring cores) 10 4 FAL07-T 4000 FAL08-2 µ, µ 10 3 µ i µ µ khz f C 260 T Amplitude permeability versus AC field flux density (measured with R29 ring cores) 000 FAL09-A µ a f = 10 khz 2 C 100 C mt 00 B Siemens Matsushita Components 87

56 N 82 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) 0 mt B 40 T = 2 C f = 10 khz FAL060-D 40 mt B 30 T = 100 C f = 10 khz FAL061-L B sat = 02 mt B r = 196 mt H c = 22 A/m 10 0 B sat = 418 mt B r = 87 mt H c = 14,6 A/m A/m 1400 H A/m 1400 H DC magnetic bias of E, ETD and U cores ( B 0,2 mt, f = 10 khz, T = 2 C) FAL062-U 000 µ rev B <_ 0,2 mt f = 10 khz T = 2 C DC magnetic bias of E, ETD and U cores ( B 0,2 mt, f = 10 khz, T = 100 C) FAL B _< 0,2 mt µ rev 1300 f = 10 khz 10 3 T = 100 C A/m 10 H A/m H 88 Siemens Matsushita Components

57 N 82 Relative core losses versus AC field flux density (measured with R29 ring cores) Relative core losses versus temperature (measured with R29 ring cores) 10 3 kw/m 3 FAL064-B kw/m 200 mt FAL06-J PV 10 2 P V mt f = 100 khz 2 C 100 C mt 2 mt f = 100 khz mt B C 120 T Relative core losses (measured with R29 ring cores) 10 4 FAL066-S 3 kw/m 200 mt 100 mt P V mt mt 2 mt 12. mt C 100 C khz 10 3 f Siemens Matsushita Components 89

58 N 62 Complex permeability (measured with R29 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R29 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped U cores) 90 Siemens Matsushita Components

59 N 62 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of E, ETD and U cores ( B 0,2 mt, f = 10 khz, T = 2 C) DC magnetic bias of E, ETD and U cores ( B 0,2 mt, f = 10 khz, T = 100 C) Siemens Matsushita Components 91

60 N 62 Relative core losses versus AC field flux density (measured with R29 ring cores) Relative core losses versus temperature (measured with R29 ring cores) Relative core losses (measured with R29 ring cores) 92 Siemens Matsushita Components

61 N 27 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E cores) Siemens Matsushita Components 93

62 N 27 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P, PM and E cores ( B 0,2 mt, f = 10 khz, T = 2 C) 94 Siemens Matsushita Components

63 N 27 Relative core losses versus AC field flux density (measured with R16 ring cores) Relative core losses versus temperature (measured with R16 ring cores) Relative core losses (measured with R16 ring cores) Siemens Matsushita Components 9

64 N 67 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E cores) 96 Siemens Matsushita Components

65 N 67 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 2 C) Siemens Matsushita Components 97

66 N 67 Relative core losses versus AC field flux density (measured with R16 ring cores) Relative core losses versus temperature (measured with R16 ring cores) Relative core losses (measured with R16 ring cores) 98 Siemens Matsushita Components

67 N 87 Complex permeability (measured with R29 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R29 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E cores) Siemens Matsushita Components 99

68 N 87 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 2 C) DC magnetic bias of P, RM, PM and E cores ( B 0,2 mt, f = 10 khz, T = 100 C) 100 Siemens Matsushita Components

69 N 87 Relative core losses versus AC field flux density (measured with R29 ring cores) Relative core losses versus temperature (measured with R29 ring cores) Relative core losses (measured with R29 ring cores) Siemens Matsushita Components 101

70 N 72 Complex permeability (measured with R29 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R29 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped U cores) 102 Siemens Matsushita Components

71 N 72 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of E cores ( B 0,2 mt, f = 10 khz, T = 2 C) DC magnetic bias of E cores ( B 0,2 mt, f = 10 khz, T = 100 C) Siemens Matsushita Components 103

72 N 72 Relative core losses versus AC field flux density (measured with R29 ring cores) Relative core losses versus temperature (measured with R29 ring cores) Relative core losses (measured with R29 ring cores) 104 Siemens Matsushita Components

73 N 41 Complex permeability (measured with R10 ring cores, B 0,2 mt) Initial permeability µ i versus temperature (measured with R10 ring cores, B 0,2 mt) Amplitude permeability versus AC field flux density (measured with ungapped E cores) Siemens Matsushita Components 10

74 N 41 (f = 10 khz, T = 2 C) (f = 10 khz, T = 100 C) DC magnetic bias of P and RM cores ( B 0,2 mt, f = 10 khz, T = 2 C) 106 Siemens Matsushita Components

75 N 41 Relative core losses versus AC field flux density (measured with R16 ring cores) Relative core losses versus temperature (measured with R16 ring cores) Relative core losses (measured with R16 ring cores) Siemens Matsushita Components 107

76 C 302 Complex permeability (measured with R20/10 ring cores, B 0,2 mt) Relative loss factor versus frequeny (measured with R20/10 ring cores, B 0,2 mt) 10 2 FAL081-1 µ s ; µ s 10 2 tan δ µ i 10 1 FAL µ µ MHz 10 3 f MHz 10 3 f 108 Siemens Matsushita Components

77 Plastic Materials Plastic materials, manufacturers and UL numbers RM coil formers of thermosetting plastic with molded-in pins: Bakelite UP 3420 [E (M)], blue; Bakelite Pinned coil formers P9, P11 7, P14 8, P18 11, EP7 special coil former: AMC 268 [E (M)], blue; Synres Almoco EP, EFD coil formers: Vyncolit/X611/green [E16721 (M)]; Vyncolit RM, EP and EFD coil formers with post-inserted pins: Vyncolit/X611/green [E16721 (M)]; Vyncolit RM coil formers with post-inserted pins: Sumikon PM 9630 [E41429 (M)]; Sumitomo Bakelite RM power, P, PM, E, EF, EC, ETD, ER coil formers and terminal carriers P7 4, P9, P11 7, P36 22: Valox 420-SE0 [E 4329 (M)], black; General Electric Plastics Vestodur GF30-FR1 [E6664 (M)], black; Creanova Crastin CE 7931 [E 6978 (M)], black; DuPont Pocan 423 [E (M)], black; Bayer Amite TV4264SN [E (M)], black; DSM Terminal carrier P4,6 4,1: Luvocom 110/GF/20/EM [---], natural; Lehmann u. Voss & Co. Terminal carriers P14 8, P18 11, P22 13, P26 16, P30 19: Pocan 423 [E (M)], gray; Bayer SMD coil formers (except of ER11 coil former): Zenite 7130 [E (M)], black; DuPont ER11 SMD coil former : Sumika Super E4008 [E 470 (M)], black; Sumitomo Chemical Zenite 7130 [E (M)], black; DuPont Rights to change material reserved. Further information is given on the packing label. The trade names are registered trademarks of the listed manufacturers. Siemens Matsushita Components 109

78 S+M COMPONENTS Siemens Matsushita Components EMI suppression capacitors Play it safe Whether video recorder, television, refrigerator or toaster our EMI suppression capacitors do a grand job in every possible kind of entertainment and consumer electronics appliance. They ve also proven their worth in switch-mode power supplies for PCs. No wonder, because the advantages of film technology are there to be seen: low cost, no risk of failure through damp, and optimum selfhealing capability. The result less destruction of equipment and ensuing fires. Plus the line is safeguarded against surges. In this way our capacitors satisfy the user s need for safety, and the new EMC standards too of course. SCS dependable, fast and competent