Initial Phase Formation During Interdiffusion

1997 ◽  
Vol 481 ◽  
Author(s):  
J. H. Perepezko ◽  
J. S. Park ◽  
K. Landry ◽  
H. Sieber ◽  
M. H. da Silva Bassani ◽  
...  

ABSTRACTIn multiphase materials systems involved in coatings, composites or multilayered structures, diffusion treatments often results in the development of intermediate phases at the reaction interfaces. While diffusional growth of phases has received much attention, the initial phase evolution involves a nucleation stage as well. The development of metastable phases during solid state interdiffusion demonstrates that the nucleation reaction can be controlling in some cases. For alloy systems with extensive solubility, intermediate phase nucleation is proceeded by interdiffusional mixing in order to achieve the required supersaturation. This leads to the identification of a critical concentration gradient for the onset of phase nucleation.The concentration gradient and the relative magnitudes of the component diffusivities provide a basis for a phase selection strategy and the application of a kinetic bias to modify the phase selection. For multicomponent alloy systems, the identification of the operative diffusion pathway is central to the control of phase formation. Experimental access to the nucleation stage of reaction is facilitated in thin film multilayer samples where the results from systems with both extensive and limited solubility offer new insight into the phase formation kinetics.

1989 ◽  
Vol 66 (4) ◽  
pp. 1674-1678 ◽  
Author(s):  
A. Suzuki ◽  
M. Nishimura ◽  
H. Yamamoto ◽  
K. Miyamoto ◽  
F. Kishi ◽  
...  

Minute ventilation (VE) during sustained hypoxia is not constant but begins to decline within 10–25 min in adult humans. The decrease in brain tissue PCO2 may be related to this decline in VE, because hypoxia causes an increase in brain blood flow, thus resulting in enhanced clearance of CO2 from the brain tissue. To examine the validity of this hypothesis, we measured VE and arterial and internal jugular venous blood gases simultaneously and repeatedly in 15 healthy male volunteers during progressive and subsequent sustained isocapnic hypoxia (arterial PO2 = 45 Torr) for 20 min. It was assumed that jugular venous PCO2 was an index of brain tissue PCO2. Mean VE declined significantly from the initial (16.5 l/min) to the final phase (14.1 l/min) of sustained hypoxia (P less than 0.05). Compared with the control (50.9 Torr), jugular venous PCO2 significantly decreased to 47.4 Torr at the initial phase of hypoxia but did not differ among the phases of hypoxia (47.2 Torr for the intermediate phase and 47.7 Torr for the final phase). We classified the subjects into two groups by hypoxic ventilatory response during progressive hypoxia at the mean value. The decrease in VE during sustained hypoxia was significant in the low responders (n = 9) [13.2 (initial phase) to 9.3 l/min (final phase of hypoxia), P less than 0.01], but not in the high responders (n = 6) (20.9–21.3 l/min, NS). This finding could not be explained by the change of arterial or jugular venous gases, which did not significantly change during sustained hypoxia in either group.(ABSTRACT TRUNCATED AT 250 WORDS)


2003 ◽  
Vol 93 (8) ◽  
pp. 4447-4453 ◽  
Author(s):  
J. Rodrı́guez-Viejo ◽  
M. Gonzalez-Silveira ◽  
M. T. Clavaguera-Mora

2000 ◽  
Vol 611 ◽  
Author(s):  
F. La Via ◽  
F. Mammoliti ◽  
M.G. Grimaldi ◽  
S. Quilici ◽  
F. Meinardi

ABSTRACTThe effect of a thin Ta layer at the Ti/Si interface on the kinetic of the C49-C54 transition will be shown in detail. The transformation kinetic has been monitored by in situ sheet resistance measurements that, coupled to structural characterisation, allowed to evidence the presence of an intermediate phase before the C54 formation. The temperature of the C54 phase formation decreases with a Ta concentration of 4.5·1015 cm−2 and μ-Raman images of partially transformed samples indicates that the density of C54 grains in presence of Ta is about one order of magnitude higher with respect to pure Ti/Si samples.


2008 ◽  
Vol 277 ◽  
pp. 47-52 ◽  
Author(s):  
Mykola Pasichnyy ◽  
Andriy Gusak

Lateral growth of intermediate phase during reactive diffusion was analyzed. Proposed model is based on the assumption that the main driving force of the lateral growth process is the chemical one (proportional to composition gradient along the interface). Asymmetric case of phase formation taking into account the curvature of all three interfaces at the triple joint is considered.


1981 ◽  
Vol 7 ◽  
Author(s):  
J. Davenas ◽  
P. Thevenard ◽  
C. Dupuy

ABSTRACTThe formation of a continuous metallic layer in the doped region of LiF crystals implanted at low temperature, has been explained by the formation of bridges between next neighbouring alkali ions of the lattice around-each implanted ion. For a critical concentration of implanted ions it is possible to show using statistical arguments that conducting chains are formed by the union of these links, according to a percolation mechanism. We show that the assumption of a distribution of isolated implanted ions at low temperature is justified by the observation of their precipitation when the crystal is warmed up to room temperature. The transformation of the metallic optical absorption into the colloidal band associated with precipitates of implanted ions is correlated with the transition from a conducting state to an insulating state of the implanted layer. We show that this evolution towards an equilibrium situation may be reversed by a reirradiation, which is used as an external perturbation and that the conducting state associated with dispersed implanted ions is then once again obtained.


1993 ◽  
Vol 8 (11) ◽  
pp. 2819-2829 ◽  
Author(s):  
M. Oehring ◽  
T. Klassen ◽  
R. Bormann

Elemental Ti–Al powder blends were mechanically alloyed in order to study phase formation during the alloying process. In addition, the stability of intermetallic phases upon milling was investigated separately in order to determine the origins of phase selection during the milling process. It was found that by mechanical alloying of powder blends, as well as by ball milling of Ti-aluminides for long milling times, the same metastable phases were formed for corresponding compositions, i.e., the hep solid solution for Al concentrations up to 60 at. % and the fcc solid solution for 75 at. % Al. X-ray diffraction (XRD) analyses indicated that the process of mechanical alloying occurred via the diffusion of Al into Ti. By lowering the milling intensity, a two-phase mixture of the hcp solid solution and the amorphous phase was observed for Ti50Al50 and confirmed by transmission electron microscopy (TEM). The results show that phase selection in the final state during mechanical alloying of Ti–Al powder blends and milling of intermetallic compounds is mainly determined by the energetic destabilization of the competing phases caused by the milling process. The destabilization is most pronounced in the case of intermetallic compounds due to the decrease in long-range order upon milling. For the final milling stage, phase formation can be predicted by considering the relative stabilities of the respective phases calculated by the CALPHAD method using the available thermodynamic data for the Ti–Al system.


1992 ◽  
Vol 7 (2) ◽  
pp. 367-373 ◽  
Author(s):  
C.V. Thompson

It is argued that interdiffusion must precede nucleation of new phases during reactions at interfaces between compositionally different phases. The relative rates at which elemental components diffuse in the reacting phases control the sequence in which phases can form, and can also strongly affect the relative nucleation rates of alloy products, especially in the transient nucleation regime. While detailed predictions of the relative nucleation rates require usually unavailable knowledge of the energies of the relevant interfaces, in some cases, knowledge of the relevant diffusivities, along with a thermodynamic analysis, can lead to predictions of likely phase formation sequences. These concepts are used to explain the association of diffusional asymmetry with systems that undergo solid state amorphization, and to specify semiquantitatively the degree of asymmetry required for solid state amorphization.


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