Authors: Ivan Campos-Silva, M. Ortíz-Domínguez, C. VillaVelázquez, R. Escobar, N. López
Abstract: This study evaluates the boron diffusion in the Fe2B phase formed at the surface of AISI
1018 steels during the paste boriding process. The treatment was carried out at temperatures of
1123, 1173, 1223 and 1273 K with 2, 4, 5, 6 and 8 h exposure times for each temperature using a 4
mm layer thickness of boron carbide paste over the material surface. The boron diffusion coefficient
Fe2B D was determined by the mass balance equation and the boride incubation time assuming that
the boride layers obey the parabolic growth law, while the boron concentration profile along the
interphase Fe2B/substrate was unknown. The boron diffusion coefficient was interpreted as a
function of the treatment temperature, obtaining the activation energy value for diffusion controlled
growth of Fe2B boride phase.
79
Authors: Vasil I. Dybkov, L.V. Goncharuk, V.G. Khoruzha, K.A. Meleshevich, A.V. Samelyuk, V.R. Sidorko
Abstract: Two boride layers were found to form at the interface of iiron-chromiium alllloys (10 and
25% Cr) or an industrial 13% Cr steel and boron at 850-950 oC and reaction times in the range 1-12
h. In the case of a Fe-10% Cr alloy and the steel, the layers are based on the FeB and Fe2B
compounds. With a Fe-25% Cr alloy, the constituent phases are FeB and CrB for the outer layer and
Fe2B and Cr2B for the inner layer. Both layers are characterized by a pronounced texture.
Diffusional growth kinetics of boride layers are close to parabolic and can alternatively be described
by a system of two non-linear differential equations, producing a good fit to the experimental data.
The temperature dependence of the layer growth-rate constants obeys a relation of the Arrhenius
type.
181
Abstract: The Ni3Sn4 intermetallic layer occurs at the interface of nickel and the saturated or
undersaturated Sn-base solder melt at 250-450 °C and dipping times of 300 to 2400 s. Mathematical
equations are proposed to evaluate the thickness of the Ni3Sn4 layer formed under conditions of
simultaneous dissolution in the undersaturated solder melt.
153
Abstract: In the present work, a kinetic study based on a diffusion model was performed by use of
both kinetics and thermodynamic data as input parameters, it was possible to evaluate the kinetic
constant at each phase interface for a biphase configuration FeB and Fe2B grown over the surfaces
of Armco Fe and Fe-Cr binary alloys at 0.5 and 4wt. %Cr by powder- pack boriding. The simulated
values of the kinetics constants by the model were compared to those found in the literature and a
good agreement was observed. For the Fe-4wt. %Cr alloy, it was found by simulation that the layer
thickness ratio between the FeB and Fe2B phases is very sensitive to the increase of temperature and
surface boron content.
318
Authors: Bo Wei Shan, Xin Lin, Lei Wei, Wei Dong Huang
Abstract: A modified cellular automaton model was proposed to simulate the dendrite growth of
alloy. Different from previous models, this model used neither an analytical equation(such as KGT
model) nor an interface solute gradient equation to solve the velocity of solid-liquid interface, but
used the interface solute and energy conservation and thermodynamic equilibrium condition to
describe the solid/liquid interface growth kinetics process. In present model, once the temperature
field and solute field were solved by finite different method in the entire domain, the material
thermodynamic properties can be substituted into four algebraic equations to easily determine the
variation of solid fraction, interface temperature and solute concentration, instead of calculating
interface moving velocity. As a result, the complexity of the calculation can be largely reduced. The
simulated dendrite growth was in a good agreement with the Lipton–Glicksman–Kurz (LGK) model
for free dendritic growth in undercooled melts.
957
Authors: E. Perez, N. Hotaling, Ashley Ewh, Dennis D. Keiser, Yong Ho Sohn
Abstract: This study examined the growth kinetics of intermetallic phases that develop in solid-tosolid
diffusion couples assembled with U-7, 10 and 12wt.%Mo vs. Al alloys (Al, Al-2wt.%Si, Al-
5wt.%Si, 4043 and 6061) after a diffusion anneal at 550°C for 24 hours. Based on interdiffusion
microstructure and integrated interdiffusion coefficients, the addition of Si into the Al matrix alloy
was observed to significantly reduce the growth rate of the intermetallic layer that primarily
consisted of (U,Mo)Al4 phase. Growth rate of the (U,Mo)Al4 intermetallic layer also increases
slightly with Mo content; however, it was not significant compared to the effect of alloying Si into
Al alloys. Growth kinetics of (U,Mo)Al4 intermetallic layer appear highly sensitive to composition
of U-Mo fuel alloy and Al cladding alloys, and must be an important criteria in alloy
development/selection for optimum fuel performance with due consideration for compositiondependent
multicomponent interdiffusion.
149
Abstract: Two borides FeB and Fe2B were found to form as separate layers at the interface between
a 13% Cr steel and boron at 850-950 oC and reaction times up to 12 h. The chromium distribution
within the boride layers is rather irregular. Its average content is 8 at. % in the FeB layer and 9 at. %
in the Fe2B layer. Both layers are characterized by a pronounced texture. The strongest reflections
are {002} and {020} for the orthorhombic FeB phase and {002} for the tetragonal Fe2B phase.
Diffusional growth kinetics of boride layers are close to parabolic and can alternatively be described
by a system of two non-linear differential equations, producing a good fit to the experimental data.
183
Abstract: A physico-chemical consideration of the interfacial interaction and diffusion resulting in
the formation of chemical compound layers at the interface of initial substances A and B is
presented. The layer-growth kinetics is shown to be much more complicated than it follows from
conventional diffusional views neglecting interfacial reactions. In the majority of multiphase binary
systems, layer occurrence appears to be sequential rather than simultaneous. Under conditions of
diffusion control, the number of simultaneously growing compound layers at the A–B interface
cannot exceed two. Multiple layers (three and more) can only form as a result of secondary
processes connected with the rupture of a diffusion couple. In such cases, great care is necessary
when calculating diffusion coefficients to avoid obtaining their physically meaningless values.
75
Authors: Kai Ming Wu, A.M. Guo, Lin Cheng
Abstract: Three-dimensional observations of proeutectoid ferrite formed at grain boundary in an
Fe-0.09%C-1.48%Mn vanadium microalloyed alloy was revealed by techniques of serial sectioning
along with computer-aided reconstruction. The ferrite allotriomorphs nucleated at grain boundary edges
were approximately prolate ellipsoids. Not all the ferrite allotriomorphs formed at grain boundary faces
were oblate ellipsoids. The growth kinetics of ferrite allotriomorphs nucleated at grain boundary edges
was greater than that of ferrite allotriomorphs nucleated at grain boundary faces.
4578
Abstract: In this work, an approach of reactive nitrogen diffusion is presented and applied to the
iron gas nitriding process. A kinetic model based on Fick's laws is used to simulate the layer growth
kinetics of a biphase configuration composed of ε and γ’ iron nitrides grown on the pure iron
substrate. This diffusional approach, under certain assumptions, reveals the influence of the
nitriding potential on the layer growth kinetics during the gas nitriding of pure iron. Some
simulation results are presented and discussed.
172