Magnetic, electrical and plastic properties of Fe76Nb2Si13B9, Fe75Ag1Nb2Si13B9 and Fe75Cu1Nb2Si13B9 amorphous alloys

Stokłosa, Z.; Rasek, J.; Kwapuliński, P.; Badura, G.; Haneczok, G.; Pająk, L.; Lelątko, J.; Kolano-Burian, Aleksandra

doi:10.1016/j.jallcom.2011.05.070

Cited by 30 publications

(21 citation statements)

References 26 publications

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“…Single layer frame shaped sensor core was made of as-quenched Fe 80 B 11 Si 9 amorphous ribbon [3]. The inner diameter of the frame was 25 mm and outer 35 mm.…”

Section: Construction Of the Sensormentioning

confidence: 99%

Magnetic Fluxgate Sensor Characteristics Modeling Using Extended Preisach Model

Frydrych

Szewczyk²,

Salach³

2014

Acta Phys. Pol. A

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This paper presents the implementation of the extended Preisach model for uxgate sensor characteristics modeling. The developed model enables the optimization of uxgate sensor parameters for a given core material. Model consists of two parts. The rst one describes magnetic characteristics of the core, while the second part calculates output signal according to sensor dimensions and electric circuit parameters. The model is easy to adapt for modeling of other devices with magnetic cores. It can be used instead of costly and time consuming prototype testing.

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“…Single layer frame shaped sensor core was made of as-quenched Fe 80 B 11 Si 9 amorphous ribbon [3]. The inner diameter of the frame was 25 mm and outer 35 mm.…”

Section: Construction Of the Sensormentioning

confidence: 99%

Magnetic Fluxgate Sensor Characteristics Modeling Using Extended Preisach Model

Frydrych

Szewczyk²,

Salach³

2014

Acta Phys. Pol. A

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“…This eect was widely investigated in soft magnetic alloys, both amorphous [2] and nanocrystaline [3] due to the possibility of development of robust force sensors [4]. Moreover, magnetoelastic eect is signicant from the point of view of development of new methods of non-destructive testing of the ferromagnetic materials, mainly steels [5].…”

Section: Introductionmentioning

confidence: 99%

Application of Extended Jiles-Atherton Model for Modelling the Influence of Stresses on Magnetic Characteristics of the Construction Steel

et al. 2014

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Paper presents the possibility of application of the Jiles-Atherton extended model to describe the magnetic characteristics of construction steel C45 under the inuence of tensile stresses. Experiment was performed on the frame-shaped samples. Then, the inuence of stresses on hysteresis loops was modelled with the Jiles-Atherton extended model. The obtained results of the modelling are consistent with results of the experimental measurements. The results of modelling create new possibilities of explanation of the physical phenomena connected with magnetisation of the magnetic materials under stresses, which is esential for the assessment of the state of the construction steel during its exploitation in industrial conditions.

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“…Malfunctions are caused by wave interference inside or between devices. Therefore wave absorber materials were needed in order to eliminate unnecessary wave frequency [1][2][3][4][5]. In this study, we investigated the magnetic properties of Ni-Zn-Cu spinel ferrite as a wave absorber.…”

Section: Introductionmentioning

confidence: 99%

Magnetic Properties of (Nia-Znb)X Cu1-X Ferrite Nanoparticle Fabricated by Sol-Gel Process

Yang

Kim

2017

Archives of Metallurgy and Materials

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In future, more mobile devices with different frequencies will be used at the same time. Therefore, it is expected that the trouble caused by wave interference between devices will be further intensified. In order to prevent this trouble, investigation of selective frequency transmission or absorption material is required. In this paper, magnetic properties of nickel-zinc-copper ferrite nano powder was researched as wave absorber. (Ni a -Zn b ) x Cu 1-x Fe 2 O 4 (NZCF) nanoparticles were fabricated by the sol-gel method. The influence of copper substitution on lattice parameter change was analyzed by X-ray diffraction (XRD), particle size was analyzed by scanning electron microscopy (SEM), and Magnetic properties analyzed by vibrating sample magnetometer (VSM). The NZCF and Nickel-zinc ferrite (NZF) lattice parameter difference was 0.028 Å and particle size was calculated as 30 nm with the XRD peak. The VSM results of (Ni 0.3 -Zn 0 . 3 ) 0.6 Cu 1-0.6 Fe 2 O 4 annealed sample at 700°C for 3hous were 58.5 emu/g (M s ), 22.8 Oe (H c ). It was the most suitable magnetic properties for wave absorber in this investigation.

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Magnetic, electrical and plastic properties of Fe76Nb2Si13B9, Fe75Ag1Nb2Si13B9 and Fe75Cu1Nb2Si13B9 amorphous alloys

Cited by 30 publications

References 26 publications

Magnetic Fluxgate Sensor Characteristics Modeling Using Extended Preisach Model

Magnetic Fluxgate Sensor Characteristics Modeling Using Extended Preisach Model

Application of Extended Jiles-Atherton Model for Modelling the Influence of Stresses on Magnetic Characteristics of the Construction Steel

Magnetic Properties of (Nia-Znb)X Cu1-X Ferrite Nanoparticle Fabricated by Sol-Gel Process

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