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Ionic interdiffusion as interaction mechanism between Al and Si 3 N 4
Author(s) -
Adabifiroozjaei Esmaeil,
Koshy Pramod,
Emadi Fahimeh,
Mofarah Sajjad S.,
Ma Hongyang,
Rastkerdar Ebad,
Lim Sean,
Webster Richard F.,
Mitchell David R.G.,
Sorrell Charles C.
Publication year - 2019
Publication title -
journal of the american ceramic society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.9
H-Index - 196
eISSN - 1551-2916
pISSN - 0002-7820
DOI - 10.1111/jace.16358
Subject(s) - diffusion , transmission electron microscopy , alloy , activation energy , crystallography , scanning electron microscope , phase (matter) , materials science , kinetics , scanning transmission electron microscopy , ionic bonding , kinetic energy , analytical chemistry (journal) , chemistry , ion , thermodynamics , nanotechnology , metallurgy , organic chemistry , physics , chromatography , quantum mechanics , composite material
Al‐Si 3 N 4 couples were heat‐treated at 850‐1150°C for 250 hours. The thickness of the interacted area was measured by scanning electron microscopy (SEM) and scanning/transmission electron microscopy (TEM/STEM). The interaction rate increases exponentially with inverse temperature, with an activation energy of 194.23 kJ/mol and diffusion pre‐coefficient of 5 × 10 −9 m 2 /s, indicating that the interaction is diffusion‐dependent. As the results showed, the interfacial area is comprised of Al alloy channels, Si precipitates, and AlN grains. Al‐Si transfer through the solid solution (Si 3‐x Al x N 4‐y ) at the interface of Al alloy and β‐Si 3 N 4 grains controls the kinetic of the interaction. When concentration of Al in solid solution exceeds a certain amount, it undergoes a topotactic phase transformation to form Al 1‐x Si x N 1+y ( viz ., AlN). Next, the Al 1‐x Si x N 1+y grains detach from the β‐Si 3 N 4 grains and subsequently new Al‐Si 3 N 4 interfaces are established. These interfaces repeat the interaction process, continuing until all the reactant is depleted. Thus, the interaction kinetics consist of a sequence of associated parabolic stages, precluding the observation of parabolic kinetics.