Amorphous & Nanocrystalline Magnetic Cores For High Frequency Electronics
AC Reactor
DC Reactor
PFC Inductors Under 6kW PFC inductor Over 6kW
Common mode chokes
MagAmp
Differential mode chokes / output inductor
Spike absorbing cores
CT's Using Amorphous Cores Transformer C-Cores
Request for quote
Amorphous magnetic
cores allow smaller, lighter and more energy efficient designs in many
high frequency applications for Invertors, UPS, ASD (Adjustable speed
drives), and Power supplies (SMPS). Amorphous metals are produced in
using a rapid solidification technology where molten metal is cast
into thin solid ribbons by cooling at a rate of one million°C/second.
Amorphous magnetic metal has high permeability due to no crystalline
magnetic anisotropy.
Nanocrystalline cores improve on standard Amorphous magnetic properties by a highly controlled annealing process to create a uniform and very fine nanocrystalline microstructure with grain sizes of ~10nm providing 1/5th the core loss of Fe based amorphous metal.
Amorphous magnetic cores have superior magnetic characteristics,
such as lower core loss, when compared with conventional crystalline magnetic
materials. These cores can offer superior design alternative when used
as the core material in the following components:
Technical advantage
Where typical ferrite cores can only operate up to a flux
saturation level (Bsat) of 0.49 Tesla, an amorphous metal core
can operate at 1.56 Tesla. Combined with operating at permeability
similar to high-end ferrites and the flexibility of manufacturing large
cores sizes these cores can be an ideal solution for many of these components.
Nanocrystalline amorphous metal offers size, core and labor
savings for various power conversion and EMC applications. |
FINEMET® FT-3K50T and FT-8K50D |
These are brand new materials produced by applying a controlled magnetic field during annealing to industry leading thin nano crystalline ribbon. This provides a material that satisfies both high saturation magnetic flux density and high permeability. Other standard features: Low core loss, Low magnetostriction, Excellent temperature characteristics and small aging effects, Excellent high frequency characteristics and the Flexibility to control magnetic properties " B-H curve shape " during annealing process.
Material
Properties
Material |
Bsat(T) |
Permeability at 10kHz |
Permeability at 100kHz |
Br/Bs |
Saturation magnetostriction, λs (X 10^-6) |
Coercive force, Hc (A/m) |
FT-3KS |
1.23 |
100,000 |
20,000 |
40 |
< 1 |
15 |
FT-3KM |
1.23 |
70,000 |
15,000 |
50 |
< 1 |
2.5 |
FT-3K50T |
1.23 |
50,000 |
31,000 |
10 |
< 1 |
1.2 |
FT-3KL |
1.23 |
27,000 |
17,000 |
5 |
< 1 |
0.6 |
FT-8K50D |
1.32 |
5,000 |
5,000 |
0.7 |
< 8 |
1.4 |
Nanocrystalline performance curves

|
Standard cores available:
Powerlite C-cores |
Three phase
designs can be done with standard single-phase
cores or a custom three-phase amorphous metal core can be constructed
in a two-piece set as shown. |
 |
 |
These amorphous cores wound in a C-core
configuration, are ideal for AC Reactors and DC inductors from 10 to 1000+
amperes. The C-core also allows for single phase and three phase transformer
designs.
Amorphous
metal C-cores allow for operation at higher frequencies at the
same flux level. Where traditional steel cores need to operate
at increasingly lower flux densities as the frequency increases.
In order to compensate for running at lower flux densities significantly
more material is needed. Even with additional material higher temperatures
still occur. Another contributor to lowering losses is the I2R of the
winding. A physically smaller amorphous core reduces your mean
length per turn, hence your I2R copper losses are lower and copper
costs are lower. Further improvements can be realized by using Nanocrystalline C-Cores. |
Winding Options |
For higher current applications these
cores open up the new options for the conductor winding process that
is not easily achievable for toroidally constructed cores:
- Copper foil
- Large gauge square conductors
Edge
or disc winding.
In each of the above options, the winding can be accomplished on a
separate mandrel and assembled onto the C-core after the winding process.
Litz is wire commonly used for high current/high frequency designs.
However, terminating litz wire for these applications can be expensive.
An alternative to consider is disc or edge winding. This involves winding
a rectangular wire that has a relatively high aspect ratio on its edge
The quasi-planar structure reduces the skin effect, but not as great
as using litz wire although greater than can be realized with similar
magnet wire or copper foil. Other advantages are: lower copper loss,
reduced DCR, smaller size, improved heat dissipation.
Higher wattage switching devices allowing operating frequencies of
10 and 20kHz are now becoming cost effective for the high power designer.
In the past traditional EI and UI laminated inductors using 3% Ni,
silicon grain oriented steel could be used with little problem. 3 percent
nickel, silicon grain oriented steel appears to be dead above 1kHz.
Special design considerations that take into account the lower flux
densities at these frequencies allow this material to be pushed beyond
its normal intended application. This however can result higher temperatures
and much larger core sizes than with a comparable amorphous core design.
These are summarized in the below chart:
Amorphous & Nanocrystalline cores for high frequency inductors verses
competitive materials
Parameters |
Nanocrystalline C-Core |
Amorphous C-Core |
Iron Powder |
6% Si Steel |
3% Si Steel |
Ferrite |
Bsat(T) |
1.23 |
1.56 |
1.0 to 1.4 |
1.2 |
1.85 |
0.35 |
Permeability |
6,000 |
3,000 |
2 to 75 |
4,100 |
1,000 |
2,500 |
Power Loss (W/Kg) |
10 |
35 |
550 |
185 |
275 |
65 |
Turns |
1 |
2 |
8 |
2 |
4 |
5 |
This design assumes 50% permeability with 50 Oe of bias, 2500 perm
ferrite was used for comparison and core determined at 20 kHz and 2
kg BAC
When comparing Iron Powder to Amorphous core. The Amorphous core will
tend to be less expensive, and have lower losses, smaller physical
size, better heat dissipation, and are mechanically rugged. The will have lower power loss and smaller however cost will be slightly higher. |
Use these tools to help you choose the best core for your DC Inductor and AC Reactor design:
DESIGN CALCULATORS
|
Standard C-Cores - Finemet® Nanocrystalline Alloy FT3 |

|
 |
Design Data:
Technical Charts
|
Magnetization curves |
For larger kilowatt power supplies, high frequency
transformers using these C-core offer higher saturation induction of
1.56 Tesla and lower losses allowing for:
- higher efficiency
- lower transformer weight
- reduced transformer volume
|
Powerlite forms |
We produce rectangular
shapes of amorphous metal cores by stacking layers of laminations
made from amorphous metal ribbon. An adhesive rated for a continuous
operating temperature of 155°C holds the laminations together.
These forms offer a unique combination of high saturation induction (1.56
T), high permeability and low core loss and can be configured into various
shapes, allowing for one large gap to be distubuted across several smaller
gaps, reducing fringing flux, and core loss. |
Possible configurations: |
 |
Hybrids can be designed using c-core sections with corresponding
bricks for unique shapes
Applications: Medium Frequency and High Power Inverters Technical
data sheet |
Toroidal Amorphous Cores |
These are offered in various amorphous metals depending on your application
DESIGN CALCULATORS
|
|
Products |
Material |
Comments |
Microlite |
Partly crystallized iron alloy |
Sizes to match industry standard 125 permeability material |
Microlite XP |
Partly crystallized iron alloy |
Sizes to match application requirements. |
Magnaperm |
Cobalt Alloy |
|
Finemet |
Nanocrystalline |
Common mode cores |
|
MicroLite® Toroidal Choke Cores |
These are Metglas® cores
manufactured with iron-based Metglas® amorphous Alloy-SA1. They offer a unique combination of high saturation induction, high permabiliity and the lowest core loss available for high frequency choke cores allowing the use of significantly smaller sizes than possible with conventional materials. Available in both coated and boxed cores. |
Coated MicroLite Cores |

|
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Boxed MicroLite Cores |
 |
 |
Applications: DC Output
Inductors; Flyback Transformers; Differential Mode in Chokes; PFC Boost
Chokes - Continuous Mode.
Links and data sheets for download
Core Data Sheet
|
MicroLiteXP® Toroidal
Cores |
This is an amorphous alloywhich
also non-crystalline in nature. Metglas® MICROLITE XP cores operate
cooler and have lower core losses than cores made of conventional crystalline
materials such as powdered iron, ferrite or sendust. MICROLITE XP's energy-efficient
properties reduce the size of powder sources for demanding applications
in the electronics industry. |
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 |
Applications: Differential
Input Inductors, PFC Inductors, Flyback transformers, and VRM Inductors.
Links and data sheets for download:
Core Data Sheet
|
MagnaPerm® High
Permeability Cores |
These cores are manufactured with cobalt-based Metglas® amorphous alloy 2714A for high frequency applications. Theses flat loop
toroidal cores offer a unique combination of ultra-high permeability,
high saturation flux density and extremely low core loss for electronic
component designers. |
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Applications: EMI Common Mode Filtering; Telecommunications and Data Communications Interface Transformers; High Accuracy Current and Pulse Transformer Ground Fault Protection Devices.
Links and data sheets for download:
Core Data Sheet
|
Metglas® Square
Loop Cores |
These cores are manufactured with cobalt-based Metglas® amorphous alloy 2714A which allow the design of MAG AMP that can operate at higher
frequencies than previously possible. Their combination of magnetic properties
enables these MAG AMP cores to provide unparalleled precision and efficiency
in output regulation. Available in both coated and boxed cores. |
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Applications: Saturable
Reactors; Magnetic Amplifiers.
Links and data sheets for download
|
Microlite
100μ |
These
cores are ideal candidates for PFC boost inductor applications in power
supply ranges from 300 to 6kW (for higher power design see Powerlite). Microlite
100μ are
tape wound amorphous toroidal cores with a small gap, which allows
the core to achieve permeabilities less than 245. The amorphous metal
core is stable over a wide temperature range and offers a design with
fewer and smaller gaps than comparable E-core ferrites. The fewer gaps
and smaller gap size greatly reduces EMC concerns from fringing flux
and stray field. Most designs can be constructed with few turns and lower
losses providing a smaller more cost effective design. In some cases
these cores maybe a good alternative for differential input inductors,
and SMPS output inductors. Various standard core sizes are available. For the ultimagte PFC boost inductor solution contact us directly on our new Advanced Amorphous A-AL material.
A-AL - Is a powder alloy "distributed gap" Amorphous core
MICROLITE 100μ Cores
vs. The Competition - Properties
Parameters |
Microlite 100m |
Iron Powder |
MPP 60m |
Kool Mu 60m |
Ferrite |
Bsat(T) |
1.56 |
1.0 to 1.4 |
.75 |
1.1 |
0.35 |
Perm |
100 |
75 |
60 |
60 |
Gap Dependent |
Power Loss (W/Kg) |
140 |
680 |
50 |
120 |
<65 |
% Permeability at 100 Oe |
75 |
25 |
50 |
45 |
Gap Dependent |
This comparison was done using 2500 perm ferrite and core loss comparison
performed at 100 kHz and 1 kGBAC
To choose the best core for your design download the PFC calculator: Executable
|
Standard Microlite 100μ Cores |
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Design Data:
Technical Charts
|
Advanced Amorphous A-AL |
These cores are manufactured by pulverizing amorphous ribbon and pressing this powder into toroidal shapes, using amorphous alloy. allowing the designer of PFC boost inductors to reduces size and power loss as compared to conventional solutons. This A-AL material is a unique in its combination of low core loss and high DC bias which enables these cores to provide unparalleled precision and efficiency. Contact us for availablity in both coated and boxed cores. |
Common
Mode Choke Coils And Cores Made With Nanocrystalline Material |
Common Mode Chokes (CMC) made with Nanocrystalline
material have superior characteristics when compared to the most commonly
used material Mn-Zn ferrite.
Higher permeability
The potential of designing a smaller CMC with the same
number or fewer turns is of interest to many designers. Nanocrystalline
materials offer this possibility by providing a complex permeability
(µr at 100kHz
and 20C), which is more than twice that of Mn-Zn ferrite. The impedance
relative permeability (µrz) is more than four times as high as
Mn-Zn ferrite. In one case this allows the designer using Nanocrystalline
material to use a core of identical size to Mn-Zn ferrite which will
produce four times higher impedance with the same number of turns. In
another case the designer can use this material to reduce the windings
by ½ and to obtain the same low frequency impedance significantly
reducing stray capacitance, as a result high frequency impedance also
becomes large.
The below charts show the higher impedance benefit of nanocrystalline
material verses Mn-Zn ferrite. |
FT-3KM nanocrystalline |
Mn-Zn ferrite |
 |
 |
Permeability legend for above charts
Real portion of complex permeability = µr’
Impedance relative permeability = µrz
Imaginary and complex permeability = µ’’
|
Comparison of magnetic
and physical properties between FINEMET® and Mn-Zn ferrite
|
FT-3KL |
FT-3KM |
Mn-Zn ferrite |
Initial permeability at 100 kHz µr’ |
20° C |
17,000 |
17,000 |
5,300 |
100° C |
15,000 |
18,000 |
7,000 |
Impedance permeability at 100 kHz µrz |
20° C |
18,500 |
26,900 |
5,300 |
100° C |
16,000 |
27,100 |
7,000 |
Saturation magnetic flux density Bs*
(T) |
20° C |
1.23 |
1.23 |
0.44 |
100° C |
1.20 |
1.20 |
0.27 |
Residual magnetic flux density Br* (T) |
20° C |
0.06 |
0.62 |
0.10 |
100° C |
0.04 |
0.59 |
0.06 |
Coercive Force Hc *(A/m) |
20° C |
0.6 |
2.5 |
8.0 |
100° C |
0.6 |
2.7 |
4.9 |
Curie temperature Tc (°C) |
570 |
570 |
150 |
Saturation magnetostriction λs
(x106) |
~0.0 |
~0.0 |
-1.1 |
Electrical resistivity ρ(µΩ.m) |
1.2 |
1.2 |
1.0x106 |
Density d(kg/m3) |
7.4x103 |
7.3x103 |
4.85x103 |
Temperature has little affect on permeability
Another
concern to many designers is the temperature dependence of many materials
used for CMC designs. Often larger cores with more turns are used to
compensate for temperature drift. Nanocrystalline material’s frequency
characteristics of impedance are not significantly affected by temperature
change. As a result, it offers high noise suppression performance over
a wide temperature range |
Mn-Zn ferrite |
FT-3KM nanocrystalline |
 |
 |
|
Single-phase
cores
For the designer interested in winding
an inductor for a specific application we have available the following
standard cores for single-phase requirements. These are toroidal
shaped tape-wound cores made from nanocrystalline amorphous metal.
The below table lists; Product code and part number for cores made
with FT-3KM material and new FT-3KM50T upgraded version of FT-3KM.
|
 |
FT-3KM - K Series
Product Code |
P/N |
Finished Dimensions (mm) |
Ac (mm2) TYP |
Lm (mm) TYP |
Wt (g) TYP |
AL value (µH/n2) |
A ±0.7 |
B ±0.7 |
C ±0.5 |
D ±0.7 |
E REF |
F REF |
G REF |
10 kHz MIN |
100 kHz ±30% |
F1AH0538 |
FT-3KM K1208A |
13.0 |
7.1 |
6.0 |
10.7 |
2.6 |
- |
1.8 |
7.7 |
30.3 |
2.9 |
18.2 |
5.8 |
F1AH0692 |
FT-3KM K1208C |
13.5 |
12.5 |
6.8 |
15.5 |
3.2 |
- |
1.5 |
13.3 |
31.7 |
4.5 |
24.0 |
8.8 |
F1AH0654 |
FT-3KM K1812A |
20.2 |
8.1 |
10.3 |
13.1 |
3.5 |
- |
2.5 |
11.3 |
47.1 |
5.8 |
14.7 |
5.3 |
F1AH0693 |
FT-3KM K1912C |
21.1 |
13.3 |
10.0 |
18.3 |
3.5 |
- |
2.5 |
24.4 |
48.9 |
13.0 |
28.2 |
10.6 |
F1AH0694 |
FT-3KM K2313D |
25.2 |
15.1 |
11.5 |
20.7 |
3.5 |
- |
2.8 |
43.9 |
57.3 |
23.0 |
41.6 |
15.3 |
F1AH0695 |
FT-3KM K2214B |
24.2 |
10.6 |
12.0 |
16.2 |
4.0 |
- |
2.8 |
22.2 |
56.5 |
13.0 |
22.2 |
8.1 |
F1AH0696 |
FT-3KM K2515D |
27.2 |
15.6 |
13.0 |
21.2 |
3.5 |
- |
2.8 |
46.3 |
62.8 |
26.0 |
41.6 |
15.3 |
F1AH0697 |
FT-3KM K2818E |
30.4 |
18.0 |
15.8 |
24.0 |
3.5 |
1.5 |
3.0 |
55.5 |
72.3 |
37.0 |
43.4 |
15.9 |
F1AH0699 |
FT-3KM K3819D |
40.4 |
15.5 |
16.8 |
23.5 |
4.0 |
2.0 |
4.0 |
87.9 |
89.5 |
68.0 |
55.5 |
20.4 |
F1AH0700 |
FT-3KM K3824G |
40.6 |
23.0 |
21.4 |
31.0 |
4.0 |
2.0 |
4.0 |
105.0 |
97.4 |
87.0 |
61.0 |
24.4 |
F1AH0701 |
FT-3KM K5328E |
56.4 |
19.0 |
24.6 |
29.0 |
5.5 |
2.0 |
5.0 |
127.5 |
114.7 |
155.0 |
62.5 |
25.0 |
FT-3K50T - K Series
Product Code |
P/N |
Finished Dimensions (mm) |
Ac
(mm2)
TYP |
Lm
(mm)
TYP |
Wt
(g)
TYP |
AL value (µH/n2) |
A
±0.7 |
B
±0.7 |
C
±0.5 |
D
±0.7 |
E
REF |
F
REF |
G
REF |
10
kHz
MIN |
100
kHz
±30% |
F1AH1128 |
FT-3K50T K1208AS |
13.7 |
7.8 |
5.5 |
11.4 |
2.6 |
- |
1.8 |
7.7 |
30.3 |
2.9 |
16.6 |
10.3 |
F1AH1129 |
FT-3K50T K1208CS |
14.2 |
13.2 |
6.3 |
16.2 |
3.0 |
- |
1.5 |
13.3 |
31.7 |
4.5 |
26.9 |
16.7 |
F1AH1130 |
FT-3K50T K1812AS |
20.9 |
8.8 |
9.8 |
13.8 |
3.5 |
- |
2.5 |
11.3 |
47.1 |
5.8 |
13.2 |
8.2 |
F1AH1131 |
FT-3K50T K1912CS |
21.8 |
14.0 |
9.5 |
19.0 |
3.5 |
- |
2.5 |
24.4 |
48.9 |
13.0 |
32.6 |
20.2 |
F1AH1132 |
FT-3K50T K2313DS |
25.9 |
15.8 |
11.0 |
21.4 |
4.0 |
- |
2.8 |
43.9 |
57.3 |
23.0 |
50.8 |
31.5 |
F1AH1133 |
FT-3K50T K2214BS |
24.9 |
11.3 |
11.5 |
16.9 |
4.0 |
- |
2.8 |
22.2 |
56.5 |
13.0 |
25.8 |
16.0 |
F1AH1134 |
FT-3K50T K2515DS |
27.9 |
16.3 |
12.5 |
21.9 |
3.5 |
- |
2.8 |
46.3 |
62.8 |
26.0 |
46.9 |
29.1 |
F1AH1135 |
FT-3K50T K2818ES |
31.1 |
18.7 |
15.3 |
24.7 |
3.5 |
1.5 |
3.0 |
55.5 |
72.3 |
37.0 |
49.0 |
30.4 |
F1AH1136 |
FT-3K50T K3819DS |
41.1 |
16.2 |
16.3 |
24.2 |
4.0 |
2.0 |
4.0 |
87.9 |
89.5 |
68.0 |
62.5 |
38.7 |
F1AH1137 |
FT-3K50T K3824GS |
41.3 |
23.7 |
20.9 |
31.7 |
4.0 |
2.0 |
4.0 |
105.0 |
97.4 |
87.0 |
67.4 |
41.8 |
F1AH1138 |
FT-3K50T K5328ES |
57.1 |
19.7 |
24.1 |
29.7 |
5.5 |
2.0 |
5.0 |
127.5 |
114.7 |
155.0 |
71.1 |
44.1 |
|
Three-phase cores
For
the designer interested in winding an inductor for a specific application
we have available the following standard cores for three-phase requirements.
These are toroidal shaped tape-wound cores made from nanocrystalline
amorphous metal. The below table lists; Product code and part number
for cores made with FT-3KM material.
|
 |
 |
FT-3KM N Series - Nanocrystalline "M Type" toroidal cores - Three phase case |
Product Code |
P/N |
Finished Dimensions (mm) |
Ac
(mm2)
TYP |
Lm
(mm)
TYP |
Wt
(g)
TYP |
AL value (µH/n2) |
A
±0.7 |
B
±0.7 |
C
±0.5 |
D
±0.7 |
E
REF |
F
REF |
G
REF |
10
kHz
MIN |
100
kHz
±30% |
F1AH0702 |
FT-3KM N2515D |
27.6 |
16.0 |
12.6 |
22.0 |
3.2 |
1.0 |
3.0 |
46.9 |
62.8 |
28 |
41.6 |
15.3 |
F1AH0703 |
FT-3KM N3320E |
35.6 |
17.4 |
19.0 |
27.0 |
3.2 |
1.5 |
4.0 |
73.1 |
73.3 |
56 |
49.7 |
19.9 |
F1AH0704 |
FT-3KM N4225E |
46.0 |
19.0 |
21.0 |
27.0 |
4.0 |
3.0 |
4.0 |
95.6 |
105.2 |
95 |
51.4 |
20.6 |
F1AH0705 |
FT-3KM N5034E |
54.0 |
19.0 |
30.0 |
29.0 |
4.0 |
- |
5.0 |
90.0 |
131.9 |
110 |
38.6 |
15.4 |
F1AH0706 |
FT-3KM N6442E |
68.0 |
19.0 |
38.0 |
29.0 |
5.0 |
- |
5.0 |
123.8 |
166.5 |
184 |
42.0 |
16.8 |
F1AH0708 |
FT-3KM N5434G |
58.0 |
25.0 |
30.0 |
47.0 |
6.2 |
8.0 |
7.0 |
150 |
138.0 |
210 |
64.1 |
24.5 |
|
Download EMC brochure for information on common mode components: |
Common Mode Inductor Cores Using Nanocrystalline Material |
If you require much larger cores for common mode chokes
with rated currents over 100Amps these cores offer you the size to solve
these RF noise problems.
They can be used for signal lines, DC power lines, and AC power lines.
Because of the low magnetostriction these core also provide low audible
noise. Cores with base plate only, require cabling with the appropriate
BIL insulation for the voltage being used. L type cores are used when
a DC offset is present, see BH curves. |
FT-3KM F Series - Nanocrystalline "M Type" toroidal cores |
Product Code |
P/N |
Finished Dimensions (mm) |
AL value(µH/n2) |
A ±0.7 |
B ±0.7 |
C ±0.5 |
Ac (mm2) TYP |
Lm (mm) TYP |
Weight (g) TYP |
10 kHz MIN |
100 kHz ±30% |
F1AH0047 |
FT-3KM F2515D |
28.0 ± 0.5 |
16.8 + 0.7 |
12.8 + 0.5 |
46.9 |
62.8 |
25 |
42.0~100.0 |
16.9 + 30% |
F1AH1139 |
FT-3KM F3020C |
31.0 ± 0.5 |
13.0 ± 0.7 |
17.4± 0.5 |
38.2 |
78.9 |
28 |
29.8~55.4 |
11.0 + 30% |
F1AH0048 |
FT-3KM F3320E |
35.8 ± 0.5 |
17.5 ± 0.7 |
17.3 ± 0.5 |
73.1 |
83.3 |
49 |
49.7~120.0 |
19.9 ± 30% |
F1AH0049 |
FT-3KM F3724E |
49.0 ± 0.5 |
17.6 ± 0.7 |
21.1 ± 0.5 |
73.1 |
95.8 |
59 |
43.0~100.0 |
17.3 ± 30% |
F1AH1140 |
FT-3KM F4032E |
42.0 |
17.0 |
29.0 |
40.8 |
111.6 |
40 |
22.5~41.8 |
8.3 ± 30% |
F1AH0050 |
FT-3KM F4424G |
46.5 ± 0.5 |
22.8 ± 0.6 |
21.1 ± 0.5 |
142.5 |
106.8 |
123 |
75.4~180 |
30.2 ± 30% |
F1AH0896 |
FT-3KM F4535G |
49.0 ± 0.5 |
25.0 ± 0.7 |
31.0 ± 0.5 |
75.0 |
125.7 |
89 |
34.0~80.0 |
13.5 ± 30% |
F1AH0897 |
FT-3KM F4627H |
50.0 ± 0.7 |
28.2 ± 1.0 |
23.4 ± 0.5 |
178.1 |
114.7 |
168 |
89.2~210.0 |
35.1 ± 30% |
F1AH0898 |
FT-3KM F6045G |
64.0 ± 0.7 |
25.0 ± 1.0 |
41.0 ± 0.7 |
112.5 |
164.9 |
162 |
39.0~90.0 |
15.4 ± 30% |
F1AH0899 |
FT-3KM F7555G |
79.0 ± 0.7 |
25.0 ± 0.7 |
51.0 ± 0.7 |
150 |
204.2 |
267 |
42.0~100.0 |
16.6 ± 30% |
F1AH0900 |
FT-3KM F10080G |
104.0 ± 0.7 |
25.0 ± 0.7 |
76.0 ± 0.7 |
138.8 |
285.1 |
336 |
30.0~65.0 |
12.0 ± 30% |
F1AH0901 |
FT-3KM F140100 |
144.0 ± 1.0 |
35.0 ± 1.0 |
96.0 ± 0.7 |
427.5 |
380.1 |
1335 |
63.0~150.0 |
24.8 ± 30% |
F1AH0024 |
FT-3KM F200160 |
204.0 ± 1.0 |
35.0 ± 1.0 |
156.0 ± 1.0 |
427.5 |
568.6 |
1875 |
42.0~100.0 |
15.1+50%,-30% |
|
M type cores with base and base plate combined |
With base plate |
Base and core combined |
 |
 |
Product Code |
P/N |
Finished dimensions in mm |
A Max |
B Max |
C Max |
D ±0.5 |
E ±0.3 |
F ±0.5 |
G ±0.5 |
H ±0.5 |
K Min |
F1AH0026 |
FT-3KM F6045GB |
95.0 |
26.0 |
78.0 |
80.0 |
12.5 |
72.0 |
50.0 |
7.0 |
39.5 |
F1AH0027 |
FT-3KM F7555GB |
121.0 |
30.0 |
100.0 |
100.0 |
- |
- |
- |
- |
50.0 |
F1AH0053 |
FT-3KM F10080GB |
161.0 |
32.0 |
122.0 |
140.0 |
- |
- |
- |
- |
75.0 |
F1AH0029 |
FT-3KM F11080GB |
181.0 |
26.0 |
131.0 |
150.0 |
12.5 |
124.0 |
100.0 |
20.0 |
74.0 |
F1AH0031 |
FT-3KM F140100PB |
181.0 |
42.0 |
162.0 |
160.0 |
- |
- |
- |
- |
95.0 |
F1AH0032 |
FT-3KM F200160PB |
241.0 |
42.0 |
217.0 |
220.0 |
- |
- |
- |
- |
155.0 |
|
Product Code |
P/N |
Ae (mm2) Typical |
Lm (mm) Typical |
Weight (g) Typical |
Applied Screw |
AL value (µH/N2) |
Shape |
I |
J |
10kHz |
100kHz |
F1AH0026 |
FT-3KM F6045GB |
112.5 |
164.9 |
193.0 |
M4 |
M5 |
39.0 ~ 90 |
15.4 ±30% |
Combined |
F1AH0027 |
FT-3KM F7555GB |
150.0 |
204.2 |
377.0 |
– |
M6 |
42.0 ~ 100 |
16.6 ±30% |
Base Plate |
F1AH0053 |
FT-3KM F10080GB |
138.8 |
285.1 |
516.0 |
– |
M6 |
30.0 ~ 65 |
12.0 ±30% |
Base Plate |
F1AH0029 |
FT-3KM F11080GB |
213.8 |
300.8 |
613.0 |
M5 |
M6 |
40.2 ~ 95 |
16.1 ±30% |
Combined |
F1AH0031 |
FT-3KM F140100PB |
427.5 |
380.1 |
1595 |
– |
M6 |
63.0 ~ 150 |
24.8 ±30% |
Base Plate |
F1AH0032 |
FT-3KM F200160PB |
427.5 |
568.6 |
2235 |
– |
M6 |
42.0 ~ 100 |
15.1 +50%,-30% |
Base Plate |
|
FT-3KL F Series - Nanocrystalline "L Type" toroidal cores |
 |
Product Code |
P/N |
Dimensions (mm) |
Ae (mm2) Typical |
Lm (mm) Typical |
Weight (g) Typical |
AL value (uH/N2) |
A |
B |
C |
10kHz |
100kHz |
F1AS3249 |
FT-3KL F2515D |
28.5 ±0.5 |
17.5 ±0.7 |
12.3 ±0.5 |
46.9 |
62.8 |
25 |
14.5 ~ 27.0 |
15.3 ±30% |
F1AS3250 |
FT-3KL F3020C |
33.1 ±0.5 |
13.0 ±0.7 |
17.4 ±0.5 |
37.6 |
79.3 |
28 |
9.7 ~ 18.5 |
10.5 ±30% |
F1AH0680 |
FT-3KL F3320E |
35.8 ±0.5 |
17.5 ±0.7 |
17.3 ±0.5 |
73.1 |
83.3 |
49 |
17.8 ~ 33.0 |
18.8 ±30% |
F1AH0681 |
FT-3KL F3724E |
40.0 ±0.5 |
17.6 ±0.7 |
21.1 ±0.5 |
73.1 |
95.8 |
59 |
15.4 ~ 28.7 |
16.3 ±30% |
F1AS3251 |
FT-3KL F4032E |
42.3 ±0.5 |
17.8 ±0.7 |
29.1 ±0.5 |
43.8 |
113.0 |
40 |
6.5 ~ 17.5 |
8.9 ±30% |
F1AS3252 |
FT-3KL F4424G |
47.1 ±0.5 |
23.4 ±0.7 |
21.0 ±0.5 |
142.5 |
106.8 |
123 |
23.0 ~ 54.2 |
28.5 ±30% |
F1AH0682 |
FT-3KL F4535G |
49.0 ±0.5 |
25.0 ±0.7 |
31.0 ±0.5 |
75 |
125.7 |
89 |
12.1 ~ 22.4 |
12.8 ±30% |
F1AS2799 |
FT-3KL F4627H |
50.7 ±0.7 |
29.2 ±0.7 |
22.9 ±0.5 |
178.1 |
114.7 |
168 |
34.1 ~ 54.4 |
33.2 ±30% |
F1AS3253 |
FT-3KL F5040G |
52.3 ±0.7 |
22.8 ±0.5 |
37.1 ±0.7 |
73.0 |
141.0 |
80 |
9.9 ~ 18.4 |
11.0 ±30% |
F1AH0683 |
FT-3KL F6045G |
64.0 ±0.7 |
25.0 ±1.0 |
41.0 ±0.7 |
107.3 |
166 |
162 |
13.1 ~ 24.3 |
13.8 ±30% |
F1AH0684 |
FT-3KL F7555G |
79.0 ±0.7 |
25.0 ±0.7 |
51.0 ±0.7 |
146.3 |
205 |
267 |
14.4 ~ 26.8 |
15.2 ±30% |
F1AH0685 |
FT-3KL F10080G |
104.0 ±0.7 |
25.0 ±0.7 |
76.0 ±0.7 |
138.8 |
285.1 |
336 |
9.8 ~ 18.3 |
10.4 ±30% |
F1AH0686 |
FT-3KL F140100 |
144.0 ±1.0 |
35.0 ±1.0 |
96.0 ±0.7 |
427.5 |
380.1 |
1335 |
22.8 ~ 42.3 |
24.0 ±30% |
F1AS3254 |
FT-3KL F200160 |
205.0 ±1.0 |
35.0 ±1.0 |
155.0 ±0.7 |
427.5 |
568.6 |
1875 |
14.4 ~ 26.8 |
16.1 ±30% |
|
L type cores
with base and base plate combined |
With base plate |
Base and core combined |
 |
 |
Product Code |
P/N |
Dimensions in mm |
A Max |
B Max |
C Max |
D ±0.5 |
E ±0.3 |
F ±0.5 |
G ±0.5 |
H ±0.5 |
K Min |
F1AH0687 |
FT-3KL F6045GB |
95.0 |
26.0 |
78.0 |
80.0 |
12.5 |
72.0 |
50.0 |
7.0 |
39.5 |
F1AH0688 |
FT-3KL F7555GB |
121.0 |
30.0 |
100.0 |
100.0 |
- |
- |
- |
- |
50.0 |
F1AH0690 |
FT-3KL F11080GB |
181.0 |
26.0 |
131.0 |
150.0 |
12.5 |
124.0 |
100.0 |
20.0 |
74.0 |
F1AH0691 |
FT-3KL F140100PB |
181.0 |
42.0 |
162.0 |
160.0 |
- |
- |
- |
- |
95.0 |
|
Product Code |
P/N |
Ae (mm2) Typical |
Lm (mm) Typical |
Weight (g) Typical |
Applied Screw |
AL value (uH/N2) |
Shape |
I |
J |
10kHz |
100kHz |
F1AH0687 |
FT-3KL F6045GB |
107.3 |
166.0 |
193.0 |
M4 |
M5 |
13.1 ~ 24.3 |
13.8 ±30% |
Combined |
F1AH0688 |
FT-3KL F7555GB |
146.3 |
205.0 |
377.0 |
- |
M6 |
14.4 ~ 26.8 |
15.2 ±30% |
Base plate |
F1AH0690 |
FT-3KL F11080GB |
213.8 |
300.8 |
613.0 |
M5 |
M6 |
14.4 ~ 26.7 |
15.2 ±30% |
Combined |
F1AH0691 |
FT-3KL F140100PB |
427.5 |
380.1 |
1595.0 |
- |
M6 |
22.8 ~ 42.3 |
24.0 ±30% |
Base plate |
|
FT-3K50T F Series - Toroidal cores |
 |
Product Code |
P/N |
Dimensions (mm) |
Ae (mm2) Typical |
Lm (mm) Typical |
Weight (g) Typical |
AL value (uH/N2) |
A |
B |
C |
10kHz |
100kHz |
F1AH1157 |
FT-3K50T F1613YS |
17.8 |
8.0 |
10.7 |
45.2 |
7.9 |
4 |
7.7 ~ 14.3 |
6.4 ±30% |
F1AH1181 |
FT-3K50T F2117DS |
23.3 |
15.3 |
13.9 |
18.9 |
59.6 |
11 |
14.7 ~ 27.3 |
12.0 ±30% |
F1AH1182 |
FT-3K50T F2515DS |
28.5 |
17.5 |
12.3 |
44.3 |
63.3 |
25 |
30.7 ~ 65.9 |
27.2 ±30% |
F1AH1183 |
FT-3K50T F3020CS |
33.1 |
13. |
17.4 |
37.6 |
79.3 |
28 |
21.6 ~ 40.2 |
17.9 ±30% |
F1AH1107 |
FT-3K50T F3320ES |
36.3 |
18.2 |
16.8 |
71.2 |
83.3 |
49 |
37.6 ~ 80.6 |
33.3 ±30% |
F1AH1108 |
FT-3K50T F3724ES |
40.5 |
18.3 |
20.6 |
71.2 |
95.8 |
60 |
33.9 ~ 62.9 |
28.1 ±30% |
F1AH1184 |
FT-3K50T F4032ES |
42.3 |
17.8 |
29.1 |
43.8 |
113.0 |
40 |
16.1 ~ 29.8 |
14.2 ±30% |
F1AH1185 |
FT-3K50T F4424GS |
47.1 |
23.4 |
21.0 |
138.8 |
106.8 |
123 |
57.1 ~ 122.4 |
50.6 ±30% |
F1AH1109 |
FT-3K50T F4535GS |
49.5 |
25.7 |
30.5 |
73.0 |
125.7 |
89 |
26.5 ~ 49.2 |
22.0 ±30% |
F1AH1186 |
FT-3K50T F4627HS |
50.7 |
29.2 |
22.9 |
173.4 |
114.7 |
164 |
66.5 ~ 142.5 |
58.9 ±30% |
F1AH1187 |
FT-3K50T F5040GS |
52.3 |
22.8 |
37.1 |
73.0 |
141.0 |
80 |
22.6 ~ 41.9 |
20.0 ±30% |
F1AH1110 |
FT-3K50T F6045GS |
64.7 |
26.0 |
40.3 |
104.4 |
166.0 |
162 |
27.6 ~ 59.2 |
24.5 ±30% |
F1AH1111 |
FT-3K50T F7555GS |
79.7 |
25.7 |
50.3 |
142.3 |
205.0 |
267 |
30.5 ~ 65.4 |
27.1 ±30% |
F1AH1112 |
FT-3K50T F10080GS |
104.7 |
25.7 |
75.3 |
138.8 |
285.1 |
336 |
20.9 ~ 44.7 |
18.5 ±30% |
F1AH1113 |
FT-3K50T F140100PS |
145.0 |
36.0 |
95.3 |
427.5 |
380.1 |
1335 |
49.5 ~ 106 |
43.8 ±30% |
|
FT-8K50D F Series - Toroidal cores |
 |
Product Code |
P/N |
Dimensions (mm) |
Ae (mm2) Typical |
Lm (mm) Typical |
Weight (g) Typical |
AL value (uH/N2) |
A |
B |
C |
10kHz |
100kHz |
F1AH1121 |
FT-8K50D F4535G |
49.5 |
25.7 |
30.5 |
75.0 |
125.7 |
89 |
3.7 ±30% |
3.7 ±30% |
F1AH1122 |
FT-8K50D F6045G |
64.7
| 26.0 |
40.3 |
107.3 |
166. |
157 |
4.1±30% |
4.0±30% |
F1AH1123 |
FT-8K50D F7555G |
79.7 |
25.7 |
50.3 |
146.3 |
200.5 |
272 |
4.5±30% |
4.4±30% |
F1AH1124 |
FT-8K50D F10080G |
104.7 |
25.7 |
75.3 |
139.5 |
286.2 |
336 |
3.1±30% |
3.0±30% |
F1AH1125 |
FT-8K50D F140100P |
145.0 |
36.0 |
95.3 |
430.9 |
382.8 |
1,350 |
7.1 ±30% |
7.0 ±30% |
F1AH1164 |
FT-8K50D F160130H |
166.9 |
30.5 |
123.9 |
292.5 |
455.5 |
1,029 |
4.0±30% |
4.0±30% |
F1AH1126 |
FT-8K50D F200160P |
205.0 |
36.0 |
155.0 |
427.5 |
568.6 |
1,930 |
4.7±30% |
4.7±30% |
|
Download EMC brochure for information on common mode components: |
New materials:
FT-3K70T 70,000 m
FT-3K34T 34,000 m
|
Wound Common Chokes Using Nanocrystalline Material |
Standard wound common mode and choke
cores are available as standard products for DC and single-phase AC power
lines (rated current from 5A to 40A), and for three-phase AC power line
(rated current from 3A to 600A). |
Single-phase horizontal mount |
Single-phase vertical mount |
 |
 |
Three-phase wound components |
Custom designs are available upon
request, for your application you can pick the standard product that
most closely meets your needs, or fill out our request form for a recommendation.
Typical applications include various portions of the power
supply / inverter such as input single and three phase noise filters, active
harmonic filters, output noise filters, DC Power Lines or Signal Lines.
|
 |
 |
Large Wound Components |
 |
|
Surge Absorbers, Beads And Cores |
Our
NANO amorphous tape-wound cores are used in (SMPS) Switched-Mode Power
Supplies, Frequency Inverters, ASD and UPS and other applications for
effective noise suppression caused by rapid changes in current. The high
pulse permeability of these cores allow excellent performance in the
suppression of reverse recovery current from the diode and ringing or
surge current from switching circuit. The Surge Absorber Cores are normally
used as single-turn choke or with very few turns
The saturation magnetic flux density is twice as high as that of Co-based
amorphous metal and three times higher than that of Ni-Zn ferrite. The
pulse permeability and the core loss are comparable to Co-based amorphous
metal. As a result, a small core made of this material offers higher
performance in suppression of surge current and voltage.
These cores also feature low core losses and a very high squareness
of the BH hysteresis loop resulting in a high inductance when the current
crosses zero. This high inductance effectively blocks reverse recovery
currents created by diodes. The material saturates at relative small
currents. Thus, spike blocking is not possible at DC currents. |
Beads |

Toroidal type bead core |
There are two types of beads leaded and non-leaded cores.
These are used for low power and excellent performance in suppression of
various kinds of current or voltage surge, such as the surge from a switching
diode |

Horizontal and vertical mounted leaded cores
|
Download EMC brochure for information on beads |
Cross Reference To Other Common Beads |
AMOBEADS® vs. FM BEADS® |
AMOBEADS® |
OD (mm) |
ID (mm) |
HT (mm) |
Total Flux (u Wb) min |
Al Value (u H/N2) min |
FM BEADS® |
OD (mm) |
ID (mm) |
HT (mm) |
Total Flux (u Wb) min |
Al Value (u H/N2) min |
AB3X2X3W |
4 |
1.5 |
4.5 |
0.9 |
3 |
FT-3AM B3X |
4 |
1.5 |
5 |
2.2 |
2 |
AB3X2X4.5W |
4 |
1.5 |
6.0 |
1.3 |
5 |
|
|
|
|
|
|
AB3X2X6W |
4 |
1.5 |
7.5 |
1.8 |
7 |
FT-3AM B3AR |
4 |
1.5 |
7 |
3.6 |
3.3 |
AB4X2X4.5W |
5 |
1.5 |
6.0 |
2.7 |
9 |
|
|
|
|
|
|
AB4X2X6W |
5 |
1.5 |
7.5 |
3.6 |
12 |
FT-3AM B4AR |
5 |
1.5 |
7 |
7.3 |
5.5 |
AB4X2X8W |
5 |
1.5 |
9.5 |
4.8 |
16 |
|
|
|
|
|
|
AMOBEADS® with lead vs. FM BEAD® with lead |
AMOBEADS® |
OD
(mm) |
LENGTH
for Leads
(mm) |
HT
for Core (mm) |
Total
Flux (u Wb) min |
Al
Value (u H/N2) min |
FM BEADS® |
OD
(mm) |
LENGTH
for Leads
(mm) |
HT
for Core (mm) |
Total
Flux (u Wb) min |
Al
Value (u H/N2) min |
LB4X2X8F |
6 |
16 |
12 |
4.8 |
16 |
FT-3AM B4ARL |
5 |
15 |
7 |
7.3 |
5.5 |
LB4X2X8U |
6 |
20 |
12 |
4.8 |
16 |
FT-3AM B4ARL |
5 |
13 |
7 |
7.3 |
5.5 |
Spikekiller® vs. Surge Absorber® (Total Flux equivalent products) |
Spikekiller® |
OD (mm) |
ID (mm) |
HT (mm) |
Total Flux (u Wb) min |
Al Value (µ H/N2) min |
Surge Absorber® |
OD (mm) |
ID (mm) |
HT (mm) |
Total Flux (u Wb) min |
Al Value (u H/N2) min |
SA7X6X4.5 |
9.0 |
4.4 |
7.5 |
1.8 |
1.1 |
|
|
|
|
|
|
SA8X6X4.5 |
10.0 |
4.4 |
7.5 |
3.6 |
2.0 |
|
|
|
|
|
|
SA10X6X4.5 |
12.3 |
4.4 |
7.5 |
7.2 |
3.3 |
FT-3AH C13X |
14.9 |
7.5 |
5.5 |
7.6 |
- |
SA14X8X4.5 |
16.3 |
6.3 |
7.5 |
10.8 |
3.6 |
FT-3AH C11A |
14.7 |
8.6 |
6.4 |
11.8 |
- |
|
Download EMC brochure for information on beads |
Cores - Nanocrystalline Amorphous |
These cores are used for medium and large power and are
toroidally wound cores which show excellent performance for the suppression
of various kinds of current or voltage surge, such as a surge from a switching
diode.
Core range in size from outside diameters of 11 to 38mm and
inside diameters of 4 to 22mm. |
 |
|
Finished dimensions (±0.3mm) |
|
2Φs (µWb) min |
OD (mm) |
ID (mm) |
HT (mm) |
Ac (cm2) |
Lm (cm) |
Mass (g) |
25°C |
120°C |
MP1005LF3S |
10.9 |
5.6 |
5.7 |
0.060 |
2.59 |
1.2 |
11.8 |
11.1 |
MP1205LF3S |
13.8 |
6.8 |
6.6 |
0.057 |
3.14 |
1.4 |
11.2 |
10.6 |
MP1303LF3S |
14.7 |
7.9 |
5.1 |
0.041 |
3.50 |
1.1 |
8.1 |
7.6 |
MP1305LF3S |
14.4 |
7.9 |
6.7 |
0.057 |
3.46 |
1.5 |
11.2 |
10.6 |
MP1405LF3S |
15.8 |
7.9 |
6.7 |
0.083 |
3.67 |
2.3 |
16.3 |
15.3 |
MP1506VF3S |
17.1 |
7.8 |
8.3 |
0.140 |
3.86 |
4.1 |
27.6 |
25.9 |
MP1603VF3S |
17.8 |
11.0 |
5.1 |
0.041 |
4.50 |
1.4 |
8.1 |
7.6 |
MP1805VF3S |
20.8 |
10.8 |
6.8 |
0.108 |
4.88 |
4.0 |
21.3 |
20.1 |
MP1903VF3S |
21.2 |
11.0 |
5.1 |
0.082 |
5.00 |
3.1 |
16.1 |
15.2 |
MP1906VF3S |
21.2 |
11.0 |
8.3 |
0.161 |
4.99 |
6.1 |
31.7 |
29.9 |
MP2303VF3S |
24.9 |
14.9 |
5.1 |
0.081 |
6.19 |
3.8 |
15.9 |
15.0 |
MP2705LF3S |
29.5 |
14.8 |
6.7 |
0.207 |
6.89 |
10.8 |
40.7 |
38.3 |
MP3210VF3S |
35 |
19.9 |
11.5 |
0.388 |
8.58 |
25.3 |
76.4 |
71.9 |
|
Total Flux equivalent products Mean magnetic path equivalent products |
MS series |
OD (mm) |
ID (mm) |
HT (mm) |
Total Flux (µ Wb) min |
Le (mm) |
Surge Absorber® |
OD (mm) |
ID (mm) |
HT (mm) |
Total Flux (µ Wb) min |
Le (mm) |
MS7X4X3W |
9.1 |
3.3 |
4.8 |
3.2 |
18.8 |
|
|
|
|
|
|
|
9.1 |
3.3 |
4.8 |
3.2 |
18.8 |
FT-3AH T8A |
9.5 |
4 |
6.6 |
11.8 |
20.4 |
MS10X7X4.5W |
11.5 |
5.8 |
6.6 |
4.7 |
26.7 |
|
|
|
|
|
|
|
11.5 |
5.8 |
6.6 |
4.7 |
26.7 |
FT-3AH C10A |
11.4 |
4.8 |
6.4 |
15.7 |
25.1 |
MS11X9W |
13.8 |
6.8 |
6.6 |
3.2 |
30.5 |
|
|
|
|
|
|
|
13.8 |
6.8 |
6.6 |
3.2 |
30.5 |
FT-3AH T12A |
13.5 |
6.6 |
6.6 |
15.7 |
31.4 |
MS12X8X4.5W |
13.8 |
6.8 |
6.6 |
6.3 |
31.4 |
FT-3AH C13X |
14.9 |
7.5 |
5.5 |
7.6 |
34.9 |
|
13.8 |
6.8 |
6.6 |
6.3 |
31.4 |
FT-3AH T12A |
13.5 |
6.6 |
6.6 |
15.7 |
31.4 |
MS15X10X4.5W |
16.8 |
8.8 |
6.6 |
7.9 |
39.3 |
FT-3AH C16X |
18.2 |
10.6 |
5.5 |
7.8 |
45.0 |
|
16.8 |
8.8 |
6.6 |
7.9 |
39.3 |
FT-3AH T15A |
16.7 |
8.3 |
6.6 |
19.7 |
39.3 |
MS16x10X6W |
17.8 |
8.8 |
8.1 |
12.6 |
40.8 |
FT-3AH C11A |
14.7 |
8.6 |
6.4 |
11.8 |
36.1 |
|
17.8 |
8.8 |
8.1 |
12.6 |
40.8 |
FT-3AH T15A |
16.7 |
8.3 |
6.6 |
19.7 |
39.3 |
MS18X12X4.5W |
19.8 |
10.8 |
6.6 |
9.5 |
47.1 |
FT-3AH T8A |
9.5 |
4.0 |
6.6 |
11.8 |
20.4 |
|
19.8 |
10.8 |
6.6 |
9.5 |
47.1 |
FT-3AH T18A |
19.7 |
6.6 |
10.3 |
23.6 |
47.1 |
MS21X14X4.5W |
22.8 |
12.8 |
6.6 |
11.0 |
55 |
FT-3AH C11A |
14.7 |
8.6 |
6.4 |
11.8 |
36.1 |
|
22.8 |
12.8 |
6.6 |
11.0 |
55 |
FT-3AH C12A |
21.3 |
12.7 |
7.5 |
15.7 |
53.4 |
MS12X8X3W |
13.7 |
6.4 |
4.8 |
4.2 |
31.4 |
|
|
|
|
|
|
|
13.7 |
6.4 |
4.8 |
4.2 |
31.4 |
FT-3AH T12A |
13.5 |
6.6 |
6.6 |
15.7 |
31.4 |
MS15X10X3W |
16.7 |
8.4 |
4.8 |
5.3 |
39.3 |
|
|
|
|
|
|
|
16.7 |
8.4 |
4.8 |
5.3 |
39.3 |
FT-3AH T15A |
16.7 |
8.3 |
6.6 |
19.7 |
39.3 |
old-MA26164.5 |
26 |
16 |
4.5 |
18 |
66 |
FT-3AH C54A |
26.5 |
11.6 |
8.5 |
16 |
58.9 |
|
|
Nanocrystalline Amorphous Metal |
 |
Nanocrystalline amorphous metal is produced by rapid
quenching a molten alloy to produce a amorphous metal and then heat treating
this alloy at higher than its crystallization temperature The alloy forms
Nanocrystalline grain size of approximately 10 nm in the amorphous metal.
|
 |
Annealing changes BH loops
M type material is done with no magnetic field applied
during annealing
M
type material is done with no magnetic field applied during annealing
We produce H and L type BH loops by annealing with magnetic fields
oriented either parallel or perpendicular to the ribbons surface.
Advantages are:
- High saturation magnetic flux density, more than 1 Tesla
- High permeability over 10,000u at 100kHz
- Excellent temperature characteristics. Very high Curie temperature
(570°C) resulting in small permeability variation (less than +/-10%)
at a temperature range of -40°C to 150°C.
- Less affected by mechanical stress. Because of the low magnetostriction
permeability and core loss changes have very small changes.
- Very low audio noise emission. Lower magnetostriction significantly
reduces audible noise emission when the voltage and current applied
to the core at audible frequency range.
|
General Informational Brochure |
How amorphous ribbon is made |
 |
The casting process Ribbon is cast in widths up to 8 inches in wide and then
is slit to width required for winding. Special winding machines wind the
ribbon in to various Toroidal, Oval and C-core shapes. Cores then are further
process via cutting, coating, annealing according to standard offering
and customer requests. |
|
CT's |
For several years now, electronic watt-hour meters have more and more
replaced the electromechanical Ferraris counters in the industrial world.
Since their advantages are self-evident, it is now foreseeable, that domestic
counters will also be substituted by electronic versions within the next
decade.
The key component of an electronic watt-hour meter is a high-precision current transformer(CT) which isolates the whole device from the mains
potential and provides the signal to be counted. By making use of modern
high permeability materials like crystalline 80% NiFe of permalloy type
(VACOPERM), Fe-based nano-crystalline VITROPERM or Co-based amorphous alloys
(VITROVAC), the CT meets the requirements of phase and amplitude-error
and linearity according the international meter standards ( e.g. IEC 61036,
ANSI C12.xx) with and without DC tolerance in a very easy and economic
way. Design support can be given with recommendations for core material,
core size, number of |
|
|
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