TY - JOUR
T1 - Numerical simulations of three-dimensional foam by the immersed boundary method
AU - Kim, Yongsam
AU - Lai, Ming Chih
AU - Peskin, Charles S.
AU - Seol, Yunchang
N1 - Funding Information:
The first author was supported by National Research Foundation of Korea Grant ( 2012R1A1A2043238 ). The second author was supported in part by National Science Council of Taiwan, Republic of China under grants NSC97-2628-M-009-007-MY3 , NSC98-2115-M-009-014-MY3 .
PY - 2014/7/15
Y1 - 2014/7/15
N2 - In this paper, we extend (Kim et al., 2010 [13]) to the three-dimensional dry foam case, i.e., a foam in which most of the volume is attributed to its gas phase. Dry foam dynamics involves the interaction between a gas and a collection of thin liquid-film internal boundaries that partitions the gas into discrete cells or bubbles. The liquid-film boundaries are flexible, contract under the influence of surface tension, and are permeable to the gas which moves across them by diffusion at a rate proportional to the local pressure difference across the boundary. Such problems are conventionally studied by assuming that the pressure is uniform within each bubble. Here, we introduce instead an immersed boundary method that takes into account the non-equilibrium fluid mechanics of the gas. To model gas diffusion across the internal liquid-film boundaries, we allow normal slip between the boundary and the gas at a velocity proportional to the (normal) force generated by the boundary surface tension. We implement this method in the three-dimensional framework, and test it by verifying the 3D generalization of the von Neumann relation, which governs the coarsening of a three-dimensional dry foam.
AB - In this paper, we extend (Kim et al., 2010 [13]) to the three-dimensional dry foam case, i.e., a foam in which most of the volume is attributed to its gas phase. Dry foam dynamics involves the interaction between a gas and a collection of thin liquid-film internal boundaries that partitions the gas into discrete cells or bubbles. The liquid-film boundaries are flexible, contract under the influence of surface tension, and are permeable to the gas which moves across them by diffusion at a rate proportional to the local pressure difference across the boundary. Such problems are conventionally studied by assuming that the pressure is uniform within each bubble. Here, we introduce instead an immersed boundary method that takes into account the non-equilibrium fluid mechanics of the gas. To model gas diffusion across the internal liquid-film boundaries, we allow normal slip between the boundary and the gas at a velocity proportional to the (normal) force generated by the boundary surface tension. We implement this method in the three-dimensional framework, and test it by verifying the 3D generalization of the von Neumann relation, which governs the coarsening of a three-dimensional dry foam.
KW - Capillary-driven motion
KW - Foam
KW - Immersed boundary method
KW - Permeability
KW - Von Neumann relation
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U2 - 10.1016/j.jcp.2014.03.016
DO - 10.1016/j.jcp.2014.03.016
M3 - Article
AN - SCOPUS:84897428725
SN - 0021-9991
VL - 269
SP - 1
EP - 21
JO - Journal of Computational Physics
JF - Journal of Computational Physics
ER -