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A boundary perturbation method to simulate nonlinear deformations of a two-dimensional bubble
Nonlinear deformations of a two-dimensional gas bubble are investigated in the framework of a Hamiltonian formulation involving surface variables alone. The Dirichlet–Neumann operator is introduced to accomplish this dimensional reduction and is expressed via a Taylor series expansion. A recursion f...
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Published in: | International journal of multiphase flow 2024-03, Vol.173, p.104749, Article 104749 |
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Main Author: | |
Format: | Article |
Language: | English |
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Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | Nonlinear deformations of a two-dimensional gas bubble are investigated in the framework of a Hamiltonian formulation involving surface variables alone. The Dirichlet–Neumann operator is introduced to accomplish this dimensional reduction and is expressed via a Taylor series expansion. A recursion formula is derived to determine explicitly each term in this Taylor series up to an arbitrary order of nonlinearity. Both analytical and numerical strategies are proposed to deal with this nonlinear free-boundary problem under forced or freely oscillating conditions. Simplified models are established in various approximate regimes, including a Rayleigh–Plesset equation for the time evolution of a purely circular pulsating bubble, and a second-order Stokes wave solution for weakly nonlinear shape oscillations that rotate steadily on the bubble surface. In addition, a numerical scheme is developed to simulate the full governing equations, by exploiting the efficient and accurate treatment of the Dirichlet–Neumann operator via the fast Fourier transform. Extensive tests are conducted to assess the numerical convergence of this operator as a function of various parameters. The performance of this direct solver is illustrated by applying it to the simulation of cycles of compression–dilatation for a purely circular bubble under uniform forcing, and to the computation of freely evolving shape distortions represented by steadily rotating waves and time-periodic standing waves. The former solutions are validated against predictions by the Rayleigh–Plesset model, while the latter solutions are compared to laboratory measurements in the case of mode-2 standing waves.
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•A lower-dimensional system is proposed for the nonlinear problem with capillarity.•The Dirichlet–Neumann operator is introduced in the Hamiltonian formulation.•A second-order Stokes solution is obtained for steadily rotating shape oscillations.•A Rayleigh–Plesset model is derived for variations in the purely circular case.•A direct numerical solver is developed based on the fast Fourier transform. |
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ISSN: | 0301-9322 1879-3533 |
DOI: | 10.1016/j.ijmultiphaseflow.2024.104749 |