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factory customized Nanocrystalline Ribbon - Fe-Based 1K107 Nanocrystalline Ribbon – Malio


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With our superb management, potent technical capability and strict quality command procedure, we go on to provide our shoppers with trustworthy high-quality, reasonable costs and outstanding services. We goal at becoming considered one of your most trustworthy partners and earning your pleasure for Magnetic Nanocrystalline Core, Transformer Core, High Frequency Nanocrystalline C Core, As a leading manufacture and exporter, we appreciate a great status inside the international markets, especially in America and Europe, because of our top high-quality and sensible charges.
factory customized Nanocrystalline Ribbon - 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 customized Nanocrystalline Ribbon - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

factory customized Nanocrystalline Ribbon - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

factory customized Nanocrystalline Ribbon - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

factory customized Nanocrystalline Ribbon - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

factory customized Nanocrystalline Ribbon - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures


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  • This supplier stick to the principle of "Quality first, Honesty as base", it is absolutely to be trust.
    5 Stars By Federico Michael Di Marco from Mauritius - 2017.10.13 10:47
    It is really lucky to meet such a good supplier, this is our most satisfied cooperation, I think we will work again!
    5 Stars By Kristin from British - 2018.12.05 13:53
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