Defect and Diffusion Forum
Vols. 283-286
Vols. 283-286
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Vol. 282
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Defect and Diffusion Forum
Vols. 280-281
Vols. 280-281
Defect and Diffusion Forum
Vol. 279
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Defect and Diffusion Forum
Vol. 278
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Defect and Diffusion Forum
Vol. 277
Vol. 277
Defect and Diffusion Forum
Vols. 273-276
Vols. 273-276
Defect and Diffusion Forum
Vol. 272
Vol. 272
Defect and Diffusion Forum
Vols. 269-271
Vols. 269-271
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Vol. 268
Vol. 268
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Vol. 267
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Defect and Diffusion Forum Vols. 273-276
Paper Title Page
Abstract: Osmotic dehydration of eggplant slices in sucrose and sodium chloride solutions at
different solution concentrations, stirring levels and time of process is studied. Water loss and solids
gain kinetics were experimentally determined and modelled using a diffusional model and
equilibrium values were predicted by means of Azuara model. Modelling was satisfactory and
involved effective coefficients of diffusion useful to quantify the different mass transfer fluxes.
413
Abstract: It is known that two main interdiffusion coefficients, ık
Dii and ık
Djj , as well as two cross
interdiffusion coefficients, ık
Dij and ık
Dji , are necessary for understanding the atomic diffusion for
ternary system. Here, k is the host element of ternary system, and i and j are solute
elements. These four interdiffusion coefficients are obtained from a series of experiments using
two kinds of ternary diffusion couples. In general, it is believed that ık
Dij and ık
Dji indicate the
same sign to each other, but there are a lot of experimental data showing that ık
Dij and ık
Dji
indicate opposite sign [1]. In such a case, the physical meaning of the cross interdiffusion
coefficient has not always been understood thoroughly. The purposes of this study are to measure
the interdiffusion coefficients by a series of experiments and to elucidate the physical meaning of
the two cross interdiffusion coefficients on the basis of the consideration about the relationship
between the thermodynamic functions and the cross interdiffusion coefficients. It is concluded
that ık
Dij exhibits the opposite sign to ık
Dji without contradicting the Onsarger’s reciprocity
theorem when the ( 2 2 )
c j ∂ G ∂c shows the opposite sign to ( 2 2 )
c i ∂ G ∂c . Here, c G is Gibbs free
energy of the ternary system.
419
Abstract: We model the grain boundary tracer diffusion problem by constructing a 3D structure
consisting of cubic grains each of equal volume. We build the structure in such a way that no four
cubes have a common edge. It is shown that the transition point between Harrison Type-A and
Type-B kinetics regimes occurs at a diffusant diffusion length roughly an order of magnitude
smaller than for the extensively studied case of parallel grain boundary slabs. For two dimensional
squares the transition point occurs at a diffusion length roughly a factor of five smaller than for
parallel grain boundary slabs. Thus we can draw the conclusion that dimensionality and geometric
shape are both important factors in the parametric analysis of the grain boundary diffusion problem.
425
Abstract: Net fluxes of vacancies commonly occur during chemical interdiffusion in alloys, ionic
conductivity and the annealing out of radiation damage. When atoms with different jump rates
diffuse in a net flux of vacancies the phenomenon of the vacancy-wind effect will occur. This
effect, first discovered by the late Dr John Manning, is a subtle phenomenon arising from a
disturbed distribution of vacancies with respect to a given moving atom or species of atom. In this
paper, the vacancy-wind effect is discussed and its visualization, performed for the first time by
computer simulation, is demonstrated.
431
Abstract: In this paper, we discuss different possible cation diffusion mechanisms in YSZ and
LSGM. Monte Carlo simulations are also reported of tracer diffusivities in LSGM for a
postulated cluster mechanism. These simulations extend earlier simulations on un-doped material.
The limits of the ratio of the diffusivities are consistent with experimental tracer diffusion
findings over a wide range of cation-vacancy exchange frequencies. We also develop
relationships between the phenomenological coefficients and use these relationships to predict
possible demixing and interdiffusion experimental outcomes.
445
Abstract: We report on the computer simulation (using molecular dynamics and lattice relaxation)
to explore tracer and chemical diffusion (carbon) kinetics in austenite at low carbon contents. It was
found by molecular dynamics simulations that the detailed balance relations are not valid for the
second nearest neighbours in the movements of the carbon interstitial atoms. The effect of a
possible split energy level at the second nearest neighbour positions is analysed from a theoretical
point of view.
455
Abstract: The presence of atomic oxygen at internal metal-ceramic oxide interfaces signifi-
cantly affects the physical properties of the interfaces which in turn affects the bulk properties
of the material. This problem is addressed for the model system Ag-MgO from a phenomenolog-
ical point of view using the finite element method. The performed parametric studies investigate
the influence of different kinetic parameters of the diffusion-segregation system.
461
Abstract: The interfacial reactions between a solidified Fe shell and Ti were investigated within the framework of steel alloying. Ti cylinders were immersed into liquid Fe for various durations and subsequently water-quenched. An Fe shell solidifies around the Ti. At the interface between Fe and Ti a reaction zone is formed. Initially it consists of a liquid eutectic layer, though in later stages all stable phases at elevated temperature can be found in the quenched microstructure. The larger part of this reaction zone is fluid at high temperature and both Ti and Fe dissolve into it. Moreover, intermetallic compound formation and mixing of Fe and Ti generate extra heat, shortening the time required for shell melt-back. The reaction zone reaches thicknesses up to 40 % of the initial sample’s radius and when the shell has completely remolten, a discontinuity in the thickness-time profile is expected. The exact morphology of the reaction zone at high temperature remains to be determined: presence of a solid layer of Fe2Ti may impede mixing in the initial stages.
467
Abstract: The TEXAS-V code was tuned for TROI-13 and used for analyzing the parametric
findings of the TROI experiments. The calculations for the melt composition are relatively similar
to the TROI experimental results, in which the melt composition has quite an effect on the steam
explosion occurrence probabilities and a steam explosion itself. The void fraction difference due to
a particle size difference appears to cause this composition dependency of a steam explosion. The
water depth effect in the TEXAS-V code seems to be consistent with the TROI experiments to some
degree. The water area effect of the TEXAS-V calculations isn’t exactly harmonious with that of the
TROI experiments. This indicates that TEXAS-V code as a 1-dimensional code or as a numerical
steam explosion has a limitation in estimating an area effect. The experimental information on the
particle size and the void fraction during mixing is very helpful for a verification of this relation.
474
Abstract: Visible photoluminescence was generated in standard soda-lime-silica glass powder,
mechanically milled in a high-energy attrition mill. The broad emission band maximum shows a
linear dependence on the exciting wavelength, suggesting the possibility to tune the PL emission.
The photoluminescence was attributed to defect generation related to unsatisfied chemical bonds due
to the high surface area. Raman scattering and ultraviolet-visible optical reflectance measurements
corroborate this assertion. Transmission electron microscopy measurements indicate that the powder
is composed by nanocrystallites with about 10-20 nanometers immersed in an amorphous media.
479