interface kinetic
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AIP Advances ◽  
2021 ◽  
Vol 11 (3) ◽  
pp. 035241
Author(s):  
Lingkang Wu ◽  
Yiying Zhu ◽  
Hao Wang ◽  
Mo Li
Keyword(s):  

2015 ◽  
Vol 91 (1) ◽  
Author(s):  
Kuo-An Wu ◽  
Ching-Hao Wang ◽  
Jeffrey J. Hoyt ◽  
Alain Karma

2013 ◽  
Vol 42 (42) ◽  
pp. 15219 ◽  
Author(s):  
Zaizhu Lou ◽  
Baibiao Huang ◽  
Zeyan Wang ◽  
Xiaoyan Qin ◽  
Xiaoyang Zhang ◽  
...  

Soft Matter ◽  
2012 ◽  
Vol 8 (37) ◽  
pp. 9642 ◽  
Author(s):  
M. Gregory Forest ◽  
Qi Wang ◽  
Xiaofeng Yang

2006 ◽  
Vol 118 ◽  
pp. 405-412
Author(s):  
Joo Youl Huh ◽  
Jong Pa Hong

An explicit, finite difference scheme was used to examine the effects of coherency stresses and interface kinetic barriers on the phase evolution of a binary, thin-film diffusion couple. Thin-films, initially consisting of alternating layers of two terminal phases, α and γ, were held at a temperature at which the formation of an intermediate phase, β, at α/γ interface was thermodynamically probable. When either the coherency stresses or interface kinetic barriers are present, the interfacial compositions become time-dependent and, thus, the formation of the thermodynamically stable β phase can be kinetically prohibited at the early stage of the evolution. Even if the initial α/γ thin-films have the same overall composition, the coherency constraint can result in different final equilibrium states depending on either the initial compositions of the α and γ phases or the relative magnitudes of the interfacial kinetic barriers. When both the coherency constraint and interfacial kinetic barriers are present, an intermediate phase can repeatedly form and disappear during the evolution.


2006 ◽  
Vol 11 (3) ◽  
pp. 295-314 ◽  
Author(s):  
A. Narimanyan ◽  
A. Muntean

This note emphasizes the application of the moving‐boundary methodology in the modelling of two processes of particular industrial relevance. The first model explains the application of the Stefan and Signorini type boundary conditions in the modelling of the thermal cutting of metals by a plasma beam, while the second model shows how interface kinetic conditions, employed within the framework of a two‐phase Stefan‐like model, can describe the dynamics of an aggressive reaction front in concrete‐based materials. Our formulations provide a conceptually new approach towards the understanding of the involved physical processes. The connection between the two models is discussed as well. It relies on the presence of non‐equilibrium conditions driving the moving interface.


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