TY - JOUR
T1 - Spontaneous formation of nanopores within a nanofilm
T2 - Phase diagram and multiple stable states
AU - Chu, Kang Ching
AU - Tsao, Yu Hao
AU - Tsao, Heng Kwong
AU - Sheng, Yu Jane
N1 - Publisher Copyright:
© 2022 Elsevier B.V.
PY - 2022/8/15
Y1 - 2022/8/15
N2 - Spontaneous formation of a nanopore within a liquid nanofilm immersed in a solvent was explored by many-body dissipative particle dynamics simulations. The nanofilm is sandwiched between two plates with circular orifices. As the liquid amount in the nanofilm changes, the menisci of the nanofilm near the orifices will be altered accordingly. The state of the nanofilm depicted by the mean curvature (H) of the meniscus depends on the apparent density (ρa) of the film and four regimes can be identified: (I) bulged film, (II) symmetric indented film, (III) asymmetric indented film, and (IV) nanopore formation. In the former two regimes, two identical convex (I) or concave (II) menisci are formed near the orifices. As ρa decreases further, the concave menisci are different on both sides of the nanofilm (III), and eventually the axis-symmetric nanopores (IV) emerge spontaneously. The relationship between H and ρa is not monotonous and involves minimum, maximum, and plain. As a result, multiple stable states are observed at the same Laplace pressure (ΔP) which relates to the mean curvature by the Young-Laplace equation. At a specific ΔP, the nanopore develops at lower ρa, while the indented film appears at higher ρa.
AB - Spontaneous formation of a nanopore within a liquid nanofilm immersed in a solvent was explored by many-body dissipative particle dynamics simulations. The nanofilm is sandwiched between two plates with circular orifices. As the liquid amount in the nanofilm changes, the menisci of the nanofilm near the orifices will be altered accordingly. The state of the nanofilm depicted by the mean curvature (H) of the meniscus depends on the apparent density (ρa) of the film and four regimes can be identified: (I) bulged film, (II) symmetric indented film, (III) asymmetric indented film, and (IV) nanopore formation. In the former two regimes, two identical convex (I) or concave (II) menisci are formed near the orifices. As ρa decreases further, the concave menisci are different on both sides of the nanofilm (III), and eventually the axis-symmetric nanopores (IV) emerge spontaneously. The relationship between H and ρa is not monotonous and involves minimum, maximum, and plain. As a result, multiple stable states are observed at the same Laplace pressure (ΔP) which relates to the mean curvature by the Young-Laplace equation. At a specific ΔP, the nanopore develops at lower ρa, while the indented film appears at higher ρa.
KW - Laplace pressure
KW - Many-body dissipative particle dynamics
KW - Multiple stable states
KW - Nanofilm
KW - Spontaneous formation of nanopores
UR - http://www.scopus.com/inward/record.url?scp=85131668300&partnerID=8YFLogxK
U2 - 10.1016/j.molliq.2022.119541
DO - 10.1016/j.molliq.2022.119541
M3 - 期刊論文
AN - SCOPUS:85131668300
SN - 0167-7322
VL - 360
JO - Journal of Molecular Liquids
JF - Journal of Molecular Liquids
M1 - 119541
ER -