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Photos are for informational purposes only. View product specification
please use latin characters
Dust cores: MOLYPERMALLOY (MPP) - MAGNETICS production.
Dust cores type: Alloy- Magnetics Molypermalloy (MPP) are toroidal cores with dissipate air gap.
They are made of:79% nickel, , 17% iron, and 4% molybdenum alloys, which allow to obtain lowest core power losses, in comparison to any other Dust material. MPP cores have many great magnetic properties like high resistivity, small hysteresis, low eddy currents, great stability after saturation. This is magnetic material, which provide low inductor power losses. MPP cores characterise with high induction and temperature stability. |
DUST CORES MAGNETICS HIGH FLUX
This are toroidal cores with dissipate air gap made from alloys: 50% nickel - 50% iron. Those cores characterise with high saturation induction.
High Flux have advantages, which make them very useful in high power, high voltage and frequency applications. Core saturation inductance is on 1.5T level, in comparison to 0.75 of standard MPP or 0.45 for ferrites. Power losses are lower than in standard type "iron Dust" cores. |
CORES KOOL Mμ®
Dust cores with dissipate air gap are made from iron alloys. They characterise with very low losses for a wide frequency range and high magnetic parameters stability.
Close to zero magnetostriction makes them ideal for elimination of arduous noises at high frequencies. In high frequency applications, losses in core made from iron alloys, may be the main reason of temperature rise. This is why, Kool Mμ cores are ideal for above applications, because their losses are smaller, and therefore their temperature rise and dimensions are much smaller. |
|
KOOL Mμ® CORES E SHAPE
E - shape cores with dissipate air gap have properties which make them useful in wide range of applications for example: PFC correction, chokes, flyback converters. Core induction saturation level 1,05 T. allows to store more energy in comparison to E shape ferrite cores, which leads to core dimensions decrease. Kool Mμ E shape cores are pricey competitive. They have great thermal properties.
|
XFLUX ™ Cores
Magnetics cores are made from: 6, 5 % silicon and iron dust. Material is resistant for high temperatures, without temperature ageing. XFLUX offers lower power losses than in normal dust cores.
XFLUX soft saturation characteristic offers advantages in comparison to ferrite cores. This cores are ideal for low and medium frequency chokes where induction on peak is not critical. |
MPP THINZ ™ or Molypermalloy dust cores are made from: 81% nickel, 17% iron and 2% molybdenum. They offer highest magnetic permeability, and high saturation inductance. They characterise with very small dimensions. They are temperature stable, and have small power losses.
Application: Magnetics dust cores are used in high power circuits, especially in impulse power supplies, filters and resonant circuits. |
MPP | HighFlux | kooi mm | XFLUX | |
---|---|---|---|---|
Permeability | 14-550 | 14-160 | 26-125 | 60 |
Losses in core | Lowest | Medium | Low | Medium |
Permeability vs DC bias | Very good | Good | Good | Best |
Saturation inductance (Bsat) | 0,75 T | 1,5 T | 1,05 T | 1,6 T |
Nickel content | 80% | 50% | 0% | 0% |
Relative costs | High | Medium | Low | Low |
Material properties
Material | Curie Temperature | Density | Thermal conductance |
---|---|---|---|
MPP | 4600C | 8,7 g/cm3 | 0,8 W/(cm x 0K) |
High Flux | 5000C | 8,2 g/cm3 | 0,8 W/(cm x 0K) |
Kool Mµ | 5000C | 7,0 g/cm3 | 0,8 W/(cm x 0K) |
Inductance and AL coefficient .
Inductance can be calculated on the geometry basses with following formula:
Coil inductance for given turn quantity is connected with nH inductance for one turn, according to following formula:
Inductance can be calculated on the geometry basses with following formula:
where:
L = Inductance µ = Magnetic permeability N = Turn count Ae = Core surface (cm2 ) Ie = Core length (cm) |
where:
L = Inductance µ = Magnetic permeability N = Turn quantity AL = coefficient (nH/T2) |
Inductance and turn quantity.
Following formula can be used for approximate calculation of dissipation flux for given inductance. It is only approximated value. The real result may be ± 50%.
where:
LLK = dissipation flux (mH) N = turn quantity Ae = Core surface (cm2 ) Ie = Core length(cm) |
Hysteresis
MPPM material
High Flux material
Kool Mµ material
XFlux material
Dimensions
Cores Kool Mµ - E shape
Marking | A [mm] | B [mm] | c [mm] | D [min] | E [min] | F [min] | L [nom] | M [min] |
---|---|---|---|---|---|---|---|---|
00K1207E (EF 12.6) | 12.70 | 6.40 | 3.56 | 4.42 | 8.89 | 3.56 | 1.78 | 2.64 |
00K1808E (EI-187) | 19.30 | 8.10 | 4.78 | 5.54 | 13.90 | 4.78 | 2.39 | 4.65 |
00K2510E (E-2425) | 25.40 | 9.53 | 6.53 | 6.22 | 18.80 | 6.22 | 3.17 | 6.25 |
00K3007E (DIN 30/7) | 30.10 | 15.01 | 7.06 | 9.70 | 19.50 | 6.96 | 5.11 | 6.46 |
00K3515E (EI-375) | 34.54 | 14.10 | 9.35 | 9.65 | 25.30 | 9.32 | 4.45 | 7.87 |
00K4017E (EE 42/11) | 42.80 | 21.10 | 10.80 | 15.00 | 30.40 | 11.90 | 5.95 | 9.27 |
00K4020E (DIN42/15) | 42.80 | 21.10 | 15.40 | 15.00 | 30.40 | 11.90 | 5.95 | 9.27 |
00K4022E (DIN42/20) | 42.80 | 21.10 | 20.00 | 15.00 | 30.40 | 11.90 | 5.95 | 9.27 |
00K4317E (EI-21) | 40.90 | 16.50 | 12.50 | 10.40 | 28.30 | 12.50 | 6.00 | 7.90 |
00K5528E (DIN55/21) | 54.90 | 27.60 | 20.60 | 18.50 | 37.50 | 16.80 | 8.38 | 10.30 |
00K5530E (DIN55/25) | 54.90 | 27.60 | 24.61 | 18.50 | 37.50 | 16.80 | 8.38 | 10.30 |
00K6527E (Metric E65) | 65.10 | 32.50 | 27.00 | 22.20 | 44.20 | 19.70 | 10.00 | 12.10 |
00K7228E (F11) | 72.39 | 27.94 | 19.05 | 17.78 | 52.63 | 19.05 | 9.52 | 16.89 |
00K8020E (Metric E80) | 80.01 | 38.10 | 19.81 | 28.14 | 59.28 | 19.81 | 9.91 | 19.81 |
00K8044E | 80.01 | 45.09 | 19.81 | 34.67 | 59.28 | 19.81 | 9.91 | 20.19 |
00K130LE | 130.3 | 32.5 | 54 | 22 | 108.4 | 20 | 10 | 44.2 |
OOK160LE | 160 | 38.1 | 39.6 | 28.1 | 138.2 | 19.8 | 9.9 | 59.3 |
Magnetic properties
Type | AL nH/Zwoje2±8% | l e [mm] | A e [mm2] | V e [mm3] | |||
---|---|---|---|---|---|---|---|
26µ | 40µ | 60µ | 90µ | ||||
00K1207E*** | - | - | - | 57 | 385 | ||
00K1808E*** | 26 | 35 | 48 | 69 | 914 | ||
00K2510E*** | 39 | 52 | 70 | 100 | 38.5 | 1 870 | |
00K3007E*** | 33 | 46 | 71 | 92 | 65.6 | 60.1 | 3 940 |
00K3515E*** | 56 | 75 | 102 | 146 | 69.4 | 84.0 | 5 830 |
00K4017E*** | 59 | 108 | 105 | 151 | 98,4 | 128 | 12 600 |
00K4020E*** | 80 | 108 | 150 | 217 | 98.4 | 183 | 18 000 |
00K4022E*** | 104 | 140 | 194 | 281 | 98.4 | 237 | 23 300 |
00K4317E*** | 88 | 119 | 163 | 234 | 77.5 | 152 | 11 800 |
00K5528E*** | 116 | 157 | 219 | NA | 123 | 350 | 43 100 |
00K5530E*** | 138 | 187 | 261 | NA | 123 | 417 | 51 400 |
00K6527E*** | 162 | 230 | 300 | NA | 147 | 540 | 79 400 |
00K7228E*** | 130 | 173 | 236 | NA | 137 | 368 | 50 300 |
00K8020E*** | 103 | 145 | 190 | NA | 185 | 389 | 72 100 |
00K8044E*** | 91 | - | - | NA | 208 | 389 | 80 910 |
00K130LE*** | 254 | -- | -- | NA | 219 | 1080 | 237 000 |
00K145LE*** | 190 | - | - | NA | 210 | 736 | 155 000 |
00K160LE*** | 180 | 273 | 778 | 212 000 |
Send an inquiry
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Dust cores: MOLYPERMALLOY (MPP) - MAGNETICS production.
Dust cores type: Alloy- Magnetics Molypermalloy (MPP) are toroidal cores with dissipate air gap.
They are made of:79% nickel, , 17% iron, and 4% molybdenum alloys, which allow to obtain lowest core power losses, in comparison to any other Dust material. MPP cores have many great magnetic properties like high resistivity, small hysteresis, low eddy currents, great stability after saturation. This is magnetic material, which provide low inductor power losses. MPP cores characterise with high induction and temperature stability. |
DUST CORES MAGNETICS HIGH FLUX
This are toroidal cores with dissipate air gap made from alloys: 50% nickel - 50% iron. Those cores characterise with high saturation induction.
High Flux have advantages, which make them very useful in high power, high voltage and frequency applications. Core saturation inductance is on 1.5T level, in comparison to 0.75 of standard MPP or 0.45 for ferrites. Power losses are lower than in standard type "iron Dust" cores. |
CORES KOOL Mμ®
Dust cores with dissipate air gap are made from iron alloys. They characterise with very low losses for a wide frequency range and high magnetic parameters stability.
Close to zero magnetostriction makes them ideal for elimination of arduous noises at high frequencies. In high frequency applications, losses in core made from iron alloys, may be the main reason of temperature rise. This is why, Kool Mμ cores are ideal for above applications, because their losses are smaller, and therefore their temperature rise and dimensions are much smaller. |
|
KOOL Mμ® CORES E SHAPE
E - shape cores with dissipate air gap have properties which make them useful in wide range of applications for example: PFC correction, chokes, flyback converters. Core induction saturation level 1,05 T. allows to store more energy in comparison to E shape ferrite cores, which leads to core dimensions decrease. Kool Mμ E shape cores are pricey competitive. They have great thermal properties.
|
XFLUX ™ Cores
Magnetics cores are made from: 6, 5 % silicon and iron dust. Material is resistant for high temperatures, without temperature ageing. XFLUX offers lower power losses than in normal dust cores.
XFLUX soft saturation characteristic offers advantages in comparison to ferrite cores. This cores are ideal for low and medium frequency chokes where induction on peak is not critical. |
MPP THINZ ™ or Molypermalloy dust cores are made from: 81% nickel, 17% iron and 2% molybdenum. They offer highest magnetic permeability, and high saturation inductance. They characterise with very small dimensions. They are temperature stable, and have small power losses.
Application: Magnetics dust cores are used in high power circuits, especially in impulse power supplies, filters and resonant circuits. |
MPP | HighFlux | kooi mm | XFLUX | |
---|---|---|---|---|
Permeability | 14-550 | 14-160 | 26-125 | 60 |
Losses in core | Lowest | Medium | Low | Medium |
Permeability vs DC bias | Very good | Good | Good | Best |
Saturation inductance (Bsat) | 0,75 T | 1,5 T | 1,05 T | 1,6 T |
Nickel content | 80% | 50% | 0% | 0% |
Relative costs | High | Medium | Low | Low |
Material properties
Material | Curie Temperature | Density | Thermal conductance |
---|---|---|---|
MPP | 4600C | 8,7 g/cm3 | 0,8 W/(cm x 0K) |
High Flux | 5000C | 8,2 g/cm3 | 0,8 W/(cm x 0K) |
Kool Mµ | 5000C | 7,0 g/cm3 | 0,8 W/(cm x 0K) |
Inductance and AL coefficient .
Inductance can be calculated on the geometry basses with following formula:
Coil inductance for given turn quantity is connected with nH inductance for one turn, according to following formula:
Inductance can be calculated on the geometry basses with following formula:
where:
L = Inductance µ = Magnetic permeability N = Turn count Ae = Core surface (cm2 ) Ie = Core length (cm) |
where:
L = Inductance µ = Magnetic permeability N = Turn quantity AL = coefficient (nH/T2) |
Inductance and turn quantity.
Following formula can be used for approximate calculation of dissipation flux for given inductance. It is only approximated value. The real result may be ± 50%.
where:
LLK = dissipation flux (mH) N = turn quantity Ae = Core surface (cm2 ) Ie = Core length(cm) |
Hysteresis
MPPM material
High Flux material
Kool Mµ material
XFlux material
Dimensions
Cores Kool Mµ - E shape
Marking | A [mm] | B [mm] | c [mm] | D [min] | E [min] | F [min] | L [nom] | M [min] |
---|---|---|---|---|---|---|---|---|
00K1207E (EF 12.6) | 12.70 | 6.40 | 3.56 | 4.42 | 8.89 | 3.56 | 1.78 | 2.64 |
00K1808E (EI-187) | 19.30 | 8.10 | 4.78 | 5.54 | 13.90 | 4.78 | 2.39 | 4.65 |
00K2510E (E-2425) | 25.40 | 9.53 | 6.53 | 6.22 | 18.80 | 6.22 | 3.17 | 6.25 |
00K3007E (DIN 30/7) | 30.10 | 15.01 | 7.06 | 9.70 | 19.50 | 6.96 | 5.11 | 6.46 |
00K3515E (EI-375) | 34.54 | 14.10 | 9.35 | 9.65 | 25.30 | 9.32 | 4.45 | 7.87 |
00K4017E (EE 42/11) | 42.80 | 21.10 | 10.80 | 15.00 | 30.40 | 11.90 | 5.95 | 9.27 |
00K4020E (DIN42/15) | 42.80 | 21.10 | 15.40 | 15.00 | 30.40 | 11.90 | 5.95 | 9.27 |
00K4022E (DIN42/20) | 42.80 | 21.10 | 20.00 | 15.00 | 30.40 | 11.90 | 5.95 | 9.27 |
00K4317E (EI-21) | 40.90 | 16.50 | 12.50 | 10.40 | 28.30 | 12.50 | 6.00 | 7.90 |
00K5528E (DIN55/21) | 54.90 | 27.60 | 20.60 | 18.50 | 37.50 | 16.80 | 8.38 | 10.30 |
00K5530E (DIN55/25) | 54.90 | 27.60 | 24.61 | 18.50 | 37.50 | 16.80 | 8.38 | 10.30 |
00K6527E (Metric E65) | 65.10 | 32.50 | 27.00 | 22.20 | 44.20 | 19.70 | 10.00 | 12.10 |
00K7228E (F11) | 72.39 | 27.94 | 19.05 | 17.78 | 52.63 | 19.05 | 9.52 | 16.89 |
00K8020E (Metric E80) | 80.01 | 38.10 | 19.81 | 28.14 | 59.28 | 19.81 | 9.91 | 19.81 |
00K8044E | 80.01 | 45.09 | 19.81 | 34.67 | 59.28 | 19.81 | 9.91 | 20.19 |
00K130LE | 130.3 | 32.5 | 54 | 22 | 108.4 | 20 | 10 | 44.2 |
OOK160LE | 160 | 38.1 | 39.6 | 28.1 | 138.2 | 19.8 | 9.9 | 59.3 |
Magnetic properties
Type | AL nH/Zwoje2±8% | l e [mm] | A e [mm2] | V e [mm3] | |||
---|---|---|---|---|---|---|---|
26µ | 40µ | 60µ | 90µ | ||||
00K1207E*** | - | - | - | 57 | 385 | ||
00K1808E*** | 26 | 35 | 48 | 69 | 914 | ||
00K2510E*** | 39 | 52 | 70 | 100 | 38.5 | 1 870 | |
00K3007E*** | 33 | 46 | 71 | 92 | 65.6 | 60.1 | 3 940 |
00K3515E*** | 56 | 75 | 102 | 146 | 69.4 | 84.0 | 5 830 |
00K4017E*** | 59 | 108 | 105 | 151 | 98,4 | 128 | 12 600 |
00K4020E*** | 80 | 108 | 150 | 217 | 98.4 | 183 | 18 000 |
00K4022E*** | 104 | 140 | 194 | 281 | 98.4 | 237 | 23 300 |
00K4317E*** | 88 | 119 | 163 | 234 | 77.5 | 152 | 11 800 |
00K5528E*** | 116 | 157 | 219 | NA | 123 | 350 | 43 100 |
00K5530E*** | 138 | 187 | 261 | NA | 123 | 417 | 51 400 |
00K6527E*** | 162 | 230 | 300 | NA | 147 | 540 | 79 400 |
00K7228E*** | 130 | 173 | 236 | NA | 137 | 368 | 50 300 |
00K8020E*** | 103 | 145 | 190 | NA | 185 | 389 | 72 100 |
00K8044E*** | 91 | - | - | NA | 208 | 389 | 80 910 |
00K130LE*** | 254 | -- | -- | NA | 219 | 1080 | 237 000 |
00K145LE*** | 190 | - | - | NA | 210 | 736 | 155 000 |
00K160LE*** | 180 | 273 | 778 | 212 000 |