Synthesis, characterization and magnetic properties of CoxCu1−x (x∼0.01–0.3) granular alloys

2015 ◽  
Vol 374 ◽  
pp. 647-654 ◽  
Author(s):  
S. Dhara ◽  
R. Roy Chowdhury ◽  
S. Lahiri ◽  
P. Ray ◽  
B. Bandyopadhyay
1990 ◽  
Vol 67 (2) ◽  
pp. 938-942 ◽  
Author(s):  
A. Gavrin ◽  
C. L. Chien

2009 ◽  
Vol 483 (1-2) ◽  
pp. 620-622 ◽  
Author(s):  
L.F. Kiss ◽  
D. Kaptás ◽  
J. Balogh ◽  
F. Tanczikó ◽  
M. Major ◽  
...  

2003 ◽  
Vol 254-255 ◽  
pp. 79-81 ◽  
Author(s):  
R Garcı́a Calderón ◽  
D.H Ucko ◽  
L Fernández Barquı́n ◽  
Q.A Pankhurst

1994 ◽  
Vol 75 (10) ◽  
pp. 6604-6606 ◽  
Author(s):  
Gang Xiao ◽  
Jian‐Qing Wang

2002 ◽  
Vol 91 (10) ◽  
pp. 8596 ◽  
Author(s):  
A. Garcı́a Prieto ◽  
M. L. Fdez-Gubieda ◽  
C. Meneghini ◽  
A. Garcı́a-Arribas

2001 ◽  
Vol 373-376 ◽  
pp. 573-576
Author(s):  
A.B. Granovsky ◽  
Nikolai S. Perov ◽  
O. Filippov ◽  
A. Rakhmanov, Jr. ◽  
J.P. Clerc ◽  
...  

2021 ◽  
pp. 132-137
Author(s):  
Сергій Сергійович Товкач

The creation of competitive engines is impossible without the development and implementation of new materials and design and technological solutions. At present, in the engines, nickel alloys obtained by directional crystallization are widely used, including monocrystalline, granular alloys. The use of various composite materials, permanent joints from dissimilar materials is constantly expanding, extensive research is being carried out to create a structure from monolithic ceramics and intermetallic compounds. The successful introduction of unconventional materials is impossible without a thorough study of their structural strength, magnetic properties, features of deformation, and destruction, taking into account the specifics of these materials when developing the design and manufacturing technology of a part or engine unit. The article discusses a software package for the optimal design of control system elements for aircraft gas turbine engines using a description of their magnetic properties. Due to the modular structure of the optimization program, various optimization procedures and calculation programs can be used. It was determined that, for the Ising model, the formation of domains with a given spread of spins at a temperature T and a vector of magnetic induction B is calculated array element using a random number generator. The number of tests L depends on the size of the sample. In the Ising model, all parts of the N*N system are contenders for testing. So, Step corresponds to the number of Monte Carlo steps. Since the parts are selected once on average, it is possible to select one particle several times or not to select it at all. Therefore, the Step value should be significantly greater than one. For a convenient implementation of a certain model, its application with a graphical magnetization interface with a different number of iterations has been considered. When executing the command file, the following should be performed: building a geometric model, building a finite element mesh, applying loads, calculating the stress-strain state (SSS), displaying the results.


Author(s):  
A.R. Pelton ◽  
A.F. Marshall ◽  
Y.S. Lee

Amorphous materials are of current interest due to their desirable mechanical, electrical and magnetic properties. Furthermore, crystallizing amorphous alloys provides an avenue for discerning sequential and competitive phases thus allowing access to otherwise inaccessible crystalline structures. Previous studies have shown the benefits of using AEM to determine crystal structures and compositions of partially crystallized alloys. The present paper will discuss the AEM characterization of crystallized Cu-Ti and Ni-Ti amorphous films.Cu60Ti40: The amorphous alloy Cu60Ti40, when continuously heated, forms a simple intermediate, macrocrystalline phase which then transforms to the ordered, equilibrium Cu3Ti2 phase. However, contrary to what one would expect from kinetic considerations, isothermal annealing below the isochronal crystallization temperature results in direct nucleation and growth of Cu3Ti2 from the amorphous matrix.


Author(s):  
June D. Kim

Iron-base alloys containing 8-11 wt.% Si, 4-8 wt.% Al, known as “Sendust” alloys, show excellent soft magnetic properties. These magnetic properties are strongly dependent on heat treatment conditions, especially on the quenching temperature following annealing. But little has been known about the microstructure and the Fe-Si-Al ternary phase diagram has not been established. In the present investigation, transmission electron microscopy (TEM) has been used to study the microstructure in a Sendust alloy as a function of temperature.An Fe-9.34 wt.% Si-5.34 wt.% Al (approximately Fe3Si0.6Al0.4) alloy was prepared by vacuum induction melting, and homogenized at 1,200°C for 5 hrs. Specimens were heat-treated in a vertical tube furnace in air, and the temperature was controlled to an accuracy of ±2°C. Thin foils for TEM observation were prepared by jet polishing using a mixture of perchloric acid 15% and acetic acid 85% at 10V and ∼13°C. Electron microscopy was performed using a Philips EM 301 microscope.


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