scholarly journals The correlation of processes of crystallization and changes of free electron density amorphous alloy powder Co80Ni20

2005 ◽  
Vol 2 (1) ◽  
pp. 57-62
Author(s):  
Aleksa Maricic ◽  
Momcilo Ristic

Great attention is being given today to investigations on the capabilities and structural changes of amorphous and nanocrystal materials. Structural changes of the amorphous cobalt and nickel alloy powder obtained by electrochemical deposition were investigated in this paper. The crystallization process, as determined by the DSC method, occurred in two steps. The temperature dependence of electrical resistively and magnetic susceptibility in isothermal and non-isothermal conditions within the temperature range of room temperature to 700?C was determined for the powder samples pressed under pressure of 800 MPa. The X-ray structural examinations results correlate with those of the DSC analysis and the electrical resistively measuring.

2013 ◽  
Vol 12 (01) ◽  
pp. 1350006
Author(s):  
AHMED E. HANNORA ◽  
FARIED F. HANNA ◽  
LOTFY K. MAREI

Mechanical alloying (MA) method has been used to produce nanocrystallite Mn -15at.% Al alloy. X-ray diffraction (XRD) patterns for the as-milled elemental α- Mn and aluminum powder samples show a mixture of α + β- MnAl phases after 20 h of milling and changes to a dominant β- MnAl phase structure after 50 h. An average crystallite size of 40 nm was determined from Hall–Williamson method analysis after 5 h of milling. Moreover, the thermal analysis results using differential thermal analysis (DTA), suggested a possible phase transformation after 20 h of milling. Isothermal treatments are carried in the temperature range of 450°C to 1000°C. Room-temperature vibrating sample magnetometer (VSM) measurements of the hysteretic response revealed that the saturation magnetization Bs and coercivity Hc for 10 h ball milled sample are ~ 2.1 emu/g and ~ 92 Oe, respectively.


2004 ◽  
Vol 36 (2) ◽  
pp. 105-112 ◽  
Author(s):  
M. Spasojevic ◽  
Aleksa Maricic ◽  
Lidija Rafailovic

Cobalt and nickel alloy powders were obtained by electrochemical deposition on a titanium cathode from an ammonium solution of cobalt and nickel sulfate. Powders of a specific chemical structure and composition, particle shape and size were obtained by an appropriate choice of electrolysis parameters, current density, deposit growth rate and solution temperature and composition. Within the current density range of 5 - 450 mAcm-2, the current density did not significantly affect the chemical composition of the powders, but had a significant effect on the particle structure, shape and size. Crystal particles formed at a current density lower than 30 mAcm-2. Amorphous powders were obtained at a current density higher than 50 mAcm-2. Structural changes of the obtained amorphous powder of 55mol.% Ni, 45 mol.% Co, pressed under the pressure of 100 MPa, were investigated by measuring the temperature dependence of electrical resistance in isothermal and non-isothermal conditions varying from room temperature to 750?C. The process of thermal stabilization of defects that appeared during pressing occurred within the temperature range of 200-390?C. The DSC method was used to determine that the powder crystallization process occurred in two stages with peak temperatures of the exothermal maximum in the first and second stage of T1 = 438?C and T2 = 573?C, respectively. A distinct correlation between the change of electrical resistance and the crystallization process was established. The reduction of electrical resistively occurs during each crystallization stage.


2009 ◽  
Vol 152-153 ◽  
pp. 75-78 ◽  
Author(s):  
V.S. Gaviko ◽  
A.G. Popov ◽  
G.V. Ivanova ◽  
N.V. Mushnikov ◽  
Y.V. Belozerov ◽  
...  

We have synthesized a novel intermetallic compound PrFe8Ga3C and studied its structure and magnetic properties. X-ray diffraction analysis revealed that the compound possesses a tetragonal BaCd11-type structure (space group I41/amd). In this structure Ga atoms occupy the same sites as Fe atoms with preferably filling the 4(b) site. Magnetization curves have been measured on the aligned powder samples. Below the Curie temperature TC = 400 K the easy magnetization direction was found to orient within the (100) plane. At 80 K the compound has a spontaneous magnetization of 97 emu/g and anisotropy constant of 4.2107 erg/cm3. At room temperature these values reduce to 78 emu/g and 4.7106 erg/cm3, respectively.


Angle-resolved X-ray photoelectron spectroscopy (X.p.s.) has been used to monitor the bombardment of (110) faces of diamond by 600 V argon ions at both room temperature and 350 °C, and the subsequent removal of the structurally damaged surface regions by oxidative erosion with microwave-excited nitric oxide at 350 °C. Ion bombardment drastically increased the width of the C Is peak (initially symmetrical and almost as sharp as that from graphite) producing a well defined two-component signal, more clearly resolved following bombardment at the higher temperature. The angular variation of the intensities of these two components, and the behaviour of the C Is signal during erosion, suggest that ion bombardment displaces many carbon atoms to sites of lower coordination, the fraction of atoms so displaced decreasing approximately exponentially with depth from a value of ca . 0.8 at the surface to ca . 0.4 at about 17 Åf depth. After erosion of all the damaged carbon, the angular variation of the signal from the underlying diamond showed pronounced structure arising from diffraction of the outgoing photoelectrons. Monitoring the Ar 2p peaks as a function of erosion time enabled experimental depth profiles to be obtained for the implanted argon. The depth scale was quantified, independently, by considerations relating to the initial rate of uptake of oxygen and from studies of the angular variations in the intensities of the X.p.s. signals. The argon concentration at adepth, z Å ,below the surface followed the function 1/(1 + 0.3 z ) quite closely down to z = 40Å (from a value of ca . 4 atomic % of the surface), regardless of the temperature of the initial bombardment; but whereas after bombardment at room temperature, argon could not be detected below ca . 60 Å, pronounced tailing of the argon distribution occurred during bombardment at 350 °C, resulting in penetration of detectable quantities of argon as deep as 150 Å. Possible explanations of this phenomenon are briefly discussed.


2012 ◽  
Vol 560-561 ◽  
pp. 3-7 ◽  
Author(s):  
Ning Wang ◽  
Shuen Hou ◽  
Hong Yun Jin

Crystallization of the basalt fibers can reduce their mechanical property. This paper is devoted to understand the crystallization behavior of basalt fiber and its control conditions. Basalt fibers were heated at 700, 750, 800, 900, 1000, 1050 °C for 2h, then cooled down to room temperature in air. The crystallization behavior of basalt fiber was investigated by means of differential thermal analysis (DTA), X-ray powder diffraction (XRD) and Fourier transform infrared spectrometry (FTIR). The results indicate that diopside and anorthite phases appeared during crystallization process and the absorption bands of heat-treated samples in FTIR spectra split and become relatively sharp.


2008 ◽  
Vol 40 (3) ◽  
pp. 333-338 ◽  
Author(s):  
S. Grujic ◽  
N. Blagojevic ◽  
M. Tosic ◽  
V. Zivanovic ◽  
J. Nikolic

Crystallization kinetics of K2O?TiO2?3GeO2 glass was investigated by differential thermal analysis (DTA). Experiments were performed on powder samples with a particle size < 0.037 mm. The glass samples were heated at different rates in the temperature range 20-750?C. The kinetic parameters, activation energy for the crystallization process, Ec and Avrami exponent, n were calculated. Powder X-ray diffraction analysis (XRD) of crystallized glass reveals the presence of crystalline K2O?TiO2?3GeO2 indicating polymorphic crystallization with interface controlled crystal growth.


1991 ◽  
Vol 6 (3) ◽  
pp. 147-152 ◽  
Author(s):  
Liu Fengchao ◽  
Zheng Bin

AbstractThe linear coefficient of thermal expansion for three silicon single-crystal samples, taken from the head, middle, and tail of the same boule, and their powder samples have been measured at room temperature by using an X-ray powder diffractometer. All samples yield the same expansion value α=2.45 (± 0.04) × 10−6 °C at 25 °C. The results of this experiment show that the linear coefficient of thermal expansion of silicon at room temperature is not dependent on its single-crystal state or its powder state.


1979 ◽  
Vol 33 (1) ◽  
pp. 51-54 ◽  
Author(s):  
B. Brachfeld ◽  
F. Cambria ◽  
M. Palumbo

A method is described for the determination of chromium in a nickel base B-Cr-Fe-Si alloy powder. The existing technique began with the melting of as received powder samples in an electric button furnace, and analysis of the solid sample by x-ray fluorescence. The procedure gave erratic quantitative results for high chromium alloys because of the segregation associated with the precipitation of chromium borides. Dilution of the as received powders with 30% nickel before melting solved the problem of chrome boride segregation, as evidenced by the concurrence of results obtained by both x-ray fluorescence and wet chemical results for chromium percentage in the alloys.


Author(s):  
Monika K. Krawczyk ◽  
Zbigniew Czapla ◽  
Adam Ingram ◽  
Andrzej Kozdraś ◽  
Tadeusz Lis ◽  
...  

On the basis of thermal analysis (DSC, DTA, DTG), single crystal X-ray diffraction experiments, dielectric studies and optical observation, it is found that the (N2H5)3[CdCl5] crystal exhibits several structural phase transitions. At room temperature, the studied crystal exhibits ferroelastic properties and undergoes phase transition from the monoclinic to the orthorhombic phase on heating above 327 K. Upon subsequent cooling, two structural phase transitions at about 323 and 319 K are observed, where the crystal adopts orthorhombic symmetry. The presented phase transitions are unique due to the fact the first heating run results in different structural changes compared to those observed during cooling and subsequent heating/cooling runs. In the studied crystal, N2H5 + ions and 1D chains built up from {CdCl5}3− units bridged by Cl atoms occur. The phase transitions observed can be associated with reorientation of cations and partial disorder of cations as well as Cl atoms.


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