hard magnetic material
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2021 ◽  
Author(s):  
Yaocen Wang ◽  
Ziyan Hao ◽  
Yan Zhang ◽  
Xiaoyu Liang ◽  
Xiaojun Bai ◽  
...  

Author(s):  
Syefira Salsabila ◽  
Lutfi Rohman ◽  
Endhah Purwandari

Fe3O4 is the strongest magnet among other iron oxides. Magnetite Fe3O4 is applied as a permanent magnet. The hysteresis curve of the permanent magnet Fe3O4 has a coercivity field that is not too large so that the material has a good chance to be applied as an absorbent material for RADAR waves. Micromagnetic simulations were carried out on Fe3O4 material in the form of thin film against hysteresis curves and ferromagnetic resonances at various thickness variations and side length variations, and the relationship was seen with changes in the bandwidth of the radar wave absorption frequency if the thickness variation of the simulated material had the same multiple as the experimental material. The thickness variations in this study were 60 nm, 90 nm, and 120 nm, where the variations in the experiment were 0.6 mm, 0.9 mm, and 1.2 mm. Micromagnetic simulation runs were performed to obtain the hysteresis curve and resonance frequency of the Fe3O4 material. The simulation results show that the resonant frequency increases with increasing thickness (fixed side length). Meanwhile, the relationship between the resonant frequency and the side length of the thin film is inversely related. Changes in the resonant frequency of Fe3O4 material are closely related to changes in the absorption frequency band of Fe3O4 material. The hysteresis curve obtained shows that the Fe3O4 material is a hard magnetic material. Changes in the resonant frequency of Fe3O4 material are closely related to changes in the absorption frequency band of Fe3O4 material. The hysteresis curve obtained shows that the Fe3O4 material is a hard magnetic material. Changes in the resonant frequency of Fe3O4 material are closely related to changes in the absorption frequency band of Fe3O4 material. The hysteresis curve obtained shows that the Fe3O4 material is a hard magnetic material.


2020 ◽  
Author(s):  
K. Ganesh ◽  
N. Pavan Kumar ◽  
Y. Suresh Reddy ◽  
G. Lalitha

2019 ◽  
Vol 10 (5) ◽  
pp. 1254-1258
Author(s):  
V. A. Zelenskii ◽  
A. B. Ankudinov ◽  
I. M. Milyaev ◽  
M. I. Alymov

Author(s):  
Salvatore Circosta ◽  
Renato Galluzzi ◽  
Nicola Amati ◽  
Angelo Bonfitto ◽  
Luis M. Castellanos Molina ◽  
...  

Measurement ◽  
2019 ◽  
Vol 135 ◽  
pp. 503-519 ◽  
Author(s):  
Shiwei Liu ◽  
Yanhua Sun ◽  
Linsong He ◽  
Xiaoyuan Jiang ◽  
Yihua Kang

2019 ◽  
pp. 51-57
Author(s):  
V. A. Zelenskii ◽  
◽  
A. B. Ankudinov ◽  
I. M. Milyaev ◽  
M. I. Alymov ◽  
...  

Actuators ◽  
2018 ◽  
Vol 7 (4) ◽  
pp. 87 ◽  
Author(s):  
Salvatore Circosta ◽  
Angelo Bonfitto ◽  
Christopher Lusty ◽  
Patrick Keogh ◽  
Nicola Amati ◽  
...  

Flywheel Energy Storage Systems are interesting solutions for energy storage, featuring advantageous characteristics when compared to other technologies. This has motivated research effort focusing mainly on cost aspects, system reliability and energy density improvement. In this context, a novel shaftless outer-rotor layout is proposed. It features a semi-hard magnetic FeCrCo 48/5 rotor coupled with two bearingless hysteresis drives. The novelty lies in the use of the semi-hard magnetic material, lending the proposed layout advantageous features thanks to its elevated mechanical strength and magnetic properties that enable the use of bearingless hysteresis drives. The paper presents a study of the proposed layout and an assessment of its energetic features. It also focuses on the modeling of the radial magnetic suspension, where the electromagnets providing the levitating forces are modeled through a one-dimensional approach. The Jiles–Atherton model is used to describe the magnetic hysteresis of the rotor material. The proposed flywheel features a mass of 61.2 kg, a storage capability of 600 Wh at the maximum speed of 18,000 rpm and achieves an energy density of 9.8 Wh/kg. The performance of the magnetic suspension is demonstrated to be satisfactory and the influence of the hysteresis of the rotor material is highlighted.


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