2021
DOI: 10.1002/pamm.202000035
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Phase Field Simulations of Wetting Based on Molecular Simulations

Abstract: Manufacturing techniques that can produce surfaces with a defined microstructure are in the focus of current research efforts. The ability to manufacture such surfaces gives rise to the need for numerical models that can predict the wetting properties of a given microstructure and can help to optimize these surfaces with respect to certain wetting properties. The present phase field (PF) model for wetting is linked to molecular dynamics (MD) simulations by the usage of the MD based perturbed Lennard‐Jones trun… Show more

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Cited by 2 publications
(3 citation statements)
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References 6 publications
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“…The free energy density f is described as f(φ,φ)badbreak=f1(φ)goodbreak+f2(φ)goodbreak=12γlgleφ2false(1φfalse)2goodbreak+34γlglefalse|φfalse|2$$\begin{equation} f(\varphi , \nabla \varphi ) = f_1(\varphi ) + f_2(\nabla \varphi ) = 12 \frac{\gamma _\mathrm{lg}}{l^e} \varphi ^2 (1-\varphi )^2 + \frac{3}{4} \gamma _\mathrm{lg} l^e |\nabla \varphi |^2 \end{equation}$$and is composed of a local term f1(φ)$f_1(\varphi )$ and a non‐local term f2(φ)$f_2(\nabla \varphi )$. In earlier works of our group, we have also used a model from molecular thermodynamics in this phase field approach [2, 5–7]. For the present concept model study, the more simple double‐well potential is used as f1(φ)$f_1(\varphi )$.…”
Section: Basic Concepts Of the Phase Field Modelmentioning
confidence: 99%
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“…The free energy density f is described as f(φ,φ)badbreak=f1(φ)goodbreak+f2(φ)goodbreak=12γlgleφ2false(1φfalse)2goodbreak+34γlglefalse|φfalse|2$$\begin{equation} f(\varphi , \nabla \varphi ) = f_1(\varphi ) + f_2(\nabla \varphi ) = 12 \frac{\gamma _\mathrm{lg}}{l^e} \varphi ^2 (1-\varphi )^2 + \frac{3}{4} \gamma _\mathrm{lg} l^e |\nabla \varphi |^2 \end{equation}$$and is composed of a local term f1(φ)$f_1(\varphi )$ and a non‐local term f2(φ)$f_2(\nabla \varphi )$. In earlier works of our group, we have also used a model from molecular thermodynamics in this phase field approach [2, 5–7]. For the present concept model study, the more simple double‐well potential is used as f1(φ)$f_1(\varphi )$.…”
Section: Basic Concepts Of the Phase Field Modelmentioning
confidence: 99%
“…and is composed of a local term 𝑓 1 (𝜑) and a non-local term 𝑓 2 (∇𝜑). In earlier works of our group, we have also used a model from molecular thermodynamics in this phase field approach [2,[5][6][7]. For the present concept model study, the more simple double-well potential is used as 𝑓 1 (𝜑).…”
Section: Basic Concepts Of the Phase Field Modelmentioning
confidence: 99%
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