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Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio


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Reliable Supplier Magnetic Core - 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:

Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures

Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio detail pictures


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We usually continually offer you the most conscientious consumer services, along with the widest variety of designs and styles with finest materials. These initiatives include the availability of customized designs with speed and dispatch for Reliable Supplier Magnetic Core - Fe-Based 1K107 Nanocrystalline Ribbon – Malio , The product will supply to all over the world, such as: Argentina, Cairo, Salt Lake City, We've been proud to supply our products and solutions to every auto fan all around the world with our flexible, fast efficient services and strictest quality control standard which has always approved and praised by customers.
  • This is a very professional wholesaler, we always come to their company for procurement, good quality and cheap.
    5 Stars By Elsa from Madras - 2018.09.29 13:24
    The sales person is professional and responsible, warm and polite, we had a pleasant conversation and no language barriers on communication.
    5 Stars By Joanne from Malta - 2017.11.29 11:09
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