2017
DOI: 10.1051/epjconf/201715105001
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Disorder trapping by rapidly moving phase interface in an undercooled liquid

Abstract: Abstract. Non-equilibrium phenomena such as the disappearance of solute drag, the origin of solute trapping and evolution of disorder trapping occur during fast transformations with originating metastable phases [D.M. Herlach, P.K. Galenko, D. Holland-Moritz, Metastable solids from undrercooled melts (Elsevier, Amsterdam, 2007)]. In the present work, a theoretical investigation of disorder trapping by a rapidly moving phase interface is presented. Using a model of fast phase transformations, a system of govern… Show more

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Cited by 1 publication
(2 citation statements)
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References 21 publications
(34 reference statements)
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“…This function might be regarded as the one modulating the free energy between two phases being modeled. The gfalse(ϕfalse)$$ g\left(\phi \right) $$ function is a wall of a simple double‐well potential [31, 39, 42, 66, 67]: pfalse(ϕfalse)=ϕ2false(32ϕfalse);0.30em0.30emgfalse(ϕfalse)=ϕ2false(1ϕfalse)2.$$ p\left(\phi \right)={\phi}^2\left(3-2\phi \right);\kern0.60em g\left(\phi \right)={\phi}^2{\left(1-\phi \right)}^2. $$ …”
Section: Modeling Of Binary Alloy Solidificationmentioning
confidence: 99%
See 1 more Smart Citation
“…This function might be regarded as the one modulating the free energy between two phases being modeled. The gfalse(ϕfalse)$$ g\left(\phi \right) $$ function is a wall of a simple double‐well potential [31, 39, 42, 66, 67]: pfalse(ϕfalse)=ϕ2false(32ϕfalse);0.30em0.30emgfalse(ϕfalse)=ϕ2false(1ϕfalse)2.$$ p\left(\phi \right)={\phi}^2\left(3-2\phi \right);\kern0.60em g\left(\phi \right)={\phi}^2{\left(1-\phi \right)}^2. $$ …”
Section: Modeling Of Binary Alloy Solidificationmentioning
confidence: 99%
“…This function might be regarded as the one modulating the free energy between two phases being modeled. The g(𝜙) function is a wall of a simple double-well potential [31,39,42,66,67]:…”
Section: Phase-field Model Of Binary Alloymentioning
confidence: 99%