Rapid nanocrystallization of soft-magnetic amorphous alloys using microwave induction heating

2009 ◽  
Vol 60 (2) ◽  
pp. 120-123 ◽  
Author(s):  
R. Nicula ◽  
M. Stir ◽  
K. Ishizaki ◽  
J.-M. Català-Civera ◽  
S. Vaucher
2016 ◽  
Vol 120 (14) ◽  
pp. 145102 ◽  
Author(s):  
Yaocen Wang ◽  
Yan Zhang ◽  
Akira Takeuchi ◽  
Akihiro Makino ◽  
Yoshiyuki Kawazoe

2007 ◽  
Vol 101 (9) ◽  
pp. 09C503 ◽  
Author(s):  
V. Franco ◽  
J. S. Blázquez ◽  
M. Millán ◽  
J. M. Borrego ◽  
C. F. Conde ◽  
...  

Microscopy ◽  
2015 ◽  
Vol 64 (suppl 1) ◽  
pp. i113.2-i113
Author(s):  
C. N. Kuo ◽  
Y. H. Chen ◽  
T. Y. Wei ◽  
Y.L. Su ◽  
J. C. Huang

Materials ◽  
2020 ◽  
Vol 13 (9) ◽  
pp. 2175 ◽  
Author(s):  
Juan Jesús Beato-López ◽  
Juan Garikoitz Urdániz-Villanueva ◽  
José Ignacio Pérez-Landazábal ◽  
Cristina Gómez-Polo

Soft magnetic amorphous alloys obtained via rapid quenching techniques are widely employed in different technological fields such as magnetic field detection, bio labeling, non-contact positioning, etc. Among them, magnetoelastic applications stand out due to excellent mechanical properties exhibited by these alloys, resulting from their amorphous structure, namely, their high Young modulus and high tensile strength. In particular, the giant stress impedance (GSI) effect represents a powerful tool to develop highly sensitive magnetoelastic sensors. This effect is based on the changes in the high-frequency electric impedance as the result of the variation in magnetic permeability of the sample under the action of mechanical stresses. In this work, the GSI effect is analyzed in two soft magnetic ribbons ((Co0.93 Fe0.07)75 Si12.5 B12.5 and (Co0.95 Fe0.05)75 Si12.5 B12.5) for the subsequent development of two practical devices: (i) the characterization of the variations in the cross-section dimensions of irregularly shaped elements, and (ii) the design of a flow meter for measuring the rate of flow of water through a pipe.


2016 ◽  
Vol 117 (10) ◽  
pp. 982-989 ◽  
Author(s):  
N. A. Skulkina ◽  
O. A. Ivanov ◽  
E. A. Stepanova ◽  
O. V. Blinova ◽  
P. A. Kuznetsov ◽  
...  

1990 ◽  
Vol 26 (5) ◽  
pp. 1424-1426 ◽  
Author(s):  
Kai-Yuan Ho ◽  
Wen-Zhi Chen ◽  
Rang-Li Gui

2018 ◽  
Vol 735 ◽  
pp. 2646-2652 ◽  
Author(s):  
Kenny L. Alvarez ◽  
José Manuel Martín ◽  
Mihail Ipatov ◽  
Julian Gonzalez

2017 ◽  
Vol 469 ◽  
pp. 27-30 ◽  
Author(s):  
Xuelian Li ◽  
Jinbao Liu ◽  
Changrong Qu ◽  
Kaikai Song ◽  
Lina Hu ◽  
...  

2005 ◽  
Vol 903 ◽  
Author(s):  
Victor A. Golubev ◽  
Andrey V. Strikanov ◽  
Aleksey V. Golubev ◽  
Vladimir G. Bugrov ◽  
Grigory A. Potemkin ◽  
...  

AbstractAt present amorphous metallic alloys have the broad expansion in various fields of science&engineering as a result of their unique properties. In particular, soft magnetic amorphous alloys are extensively used in electrical engineering. However the production of considerable-size nonporous wares based on the powders (or tapes) of these alloys is heavy problem owing to high hardness of the particles. Therefore shock wave’s compacting or Dynamic Compacting (DC) method is promising one to produce the wares on the base of powders of amorphous alloys because it can provides high strength and near zero porosity of the wares. The experimental D-U diagrams of soft magnetic amorphous alloys were obtained to realize this method of compacting. The calculations of the amplitude and duration of shock wave were carried out. The several versions of explosive devices using shock plane wave generator to produce circular magnetic conductors were developed and were tested. These magnetic conductors are based on amorphous alloys of 5BDSR, GM414, 10NSR trademarks (Fe with Cu, Nb, Si, B additives). XRD analysis proved that amorphous state of the alloys remains the same up to 20 GPa shock wave’s pressures. The mechanical, structural, electrical and magnetic properties both initial amorphous alloys and compacted one were obtained and compared as a result of the implemented works. It was stated that DC leads to increase of magnetic conductivity by factor ∼15 with respect to initial amorphous alloys powder. Besides the specific losses decrease in ∼4 times.


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