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Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio


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Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio Detail:

Description

Product Name Fe-Based 1K107 Nanocrystalline Ribbon
P/N MLNR-2132
Width 5-65mm
Thickness 26-34μm
Saturation magnetic induction 1.25  Bs (T)
Coercivity  1.5  Hc (A/m)
Resistivity 1.20 (μΩ·m )
Magnetostriction coefficient 1 λs (ppm)
Curie temperature 570  Tc (℃)
Crystallization temperature 500  Tx (℃)
Density 7.2 ρ (g/cm3)
Hardness 880
Thermal expansion coefficient 7.6

Application

● Switching power supply transformers and pulse transformer cores

● Power transformers, precision current transformer cores

● Leakage protection switch transformer iron core

● Filter inductors, energy storage inductors, reactor cores

● EMC common mode and differential mode inductor core

● Saturation reactors, magnetic amplifiers, spike suppressor cores and magnetic beads

Features

Fe-based Nanocrystalline materials are superior to conventional materials and will be the best solution for your application (Figure 1.1).

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Figure 1.1 μr versus Bs of different soft magnetic materials

● High saturation magnetic induction (1.25 T) and high magnetic permeability (>80,000) for small volumes and high precision

● Core loss equivalent to 1/5 of iron-based amorphous, with losses as low as 70 W/kg at 100 kHZ, 300 mT

● Saturation magnetostriction coefficient close to 0, with very low operating noise

● Excellent temperature stability, <10% change in material properties over the temperature range -50 to 120 °C

● Excellent frequency characteristics with excellent permeability and low losses over a wide frequency range

● With adjustable magnetic properties, different types of magnetic properties can be obtained by applying different transverse and vertical magnetic fields, or without magnetic field heat treatment, such as low remanence, high rectangular ratio, and high magnetic permeability

Material comparison

Performance Comparison of Fe-based Nanocrystalline Ribbon with Ferrite Core

Basic parameters

Nanocrystalline Ribbon

Ferrite Core
Saturation magnetic induction Bs (T)

1.25

0.5

Residual magnetic induction Br (T)(20KHz) <0.2 0.2
Core losses   (20KHz/0.2T)(W/kg) <3.4 7.5
Core losses   (20KHz/0.5T)(W/kg) <35 Cannot be used
Core losses   (50KHz/0.3T)(W/kg) <40 Cannot be used
Magnetic Conductivity (20KHz) (Gs/Oe) >20000 2000
Coercive force Hc (A/m) <2.0 6
Resistivity (mW-cm) <2 4
Saturated magnetostriction coefficient(X10-6 400 740
Resistivity(mW-cm) 80 106
Curie Temperature >0.7 -

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Product detail pictures:

Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures


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We have our own sales team, design team, technical team, QC team and package team. We have strict quality control procedures for each process. Also, all of our workers are experienced in printing field for Factory wholesale Bushing Ct - Fe-Based 1K107 Nanocrystalline Ribbon – Malio , The product will supply to all over the world, such as: Sri Lanka, Zurich, Muscat, Our items are widely recognized and trusted by users and can meet continuously developing economic and social needs. We welcome new and old customers from all walks of life to contact us for future business relationships and achieving mutual success!
  • We have been engaged in this industry for many years, we appreciate the work attitude and production capacity of the company, this is a reputable and professional manufacturer.
    5 Stars By Nancy from Bahrain - 2018.12.10 19:03
    We are long-term partners, there is no disappointment every time, we hope to maintain this friendship later!
    5 Stars By Alexandra from Southampton - 2017.08.16 13:39
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