2021
DOI: 10.32604/cmes.2021.017404
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A Hybrid Immersed Boundary/Coarse-Graining Method for Modeling Inextensible Semi-Flexible Filaments in Thermally Fluctuating Fluids

Abstract: A new and computationally efficient version of the immersed boundary method, which is combined with the coarse-graining method, is introduced for modeling inextensible filaments immersed in low-Reynolds number flows. This is used to represent actin biopolymers, which are constituent elements of the cytoskeleton, a complex network-like structure that plays a fundamental role in shape morphology. An extension of the traditional immersed boundary method to include a stochastic stress tensor is also proposed in or… Show more

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Cited by 2 publications
(1 citation statement)
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“…Moreau et al [12] highlighted the high efficiency of the formalism in two dimensions (2D), and showed excellent agreement with classical formulations, even for relatively large CG segments. Following this, the CG method has gained momentum, and was adopted and generalized in several ways: (i) non-local hydrodynamics have been accounted for passive and active filaments in 2D, including wall interactions [27][28][29], (ii) 3D filament deformations were accounted for in [30,31], though limited to a local hydrodynamic resistive force theory (RFT), as in [12], (iii) it has been applied to study sperm flagellum propulsion in 2D [32], (iv) expanded into a hybrid immersed boundary method [33], as well as a stochastic method [34], and (v) used for analytical and numerical study of the well-posedness of Newtonian and viscoelastic elastohydrodynamic propulsion [35,36].…”
Section: Introductionmentioning
confidence: 99%
“…Moreau et al [12] highlighted the high efficiency of the formalism in two dimensions (2D), and showed excellent agreement with classical formulations, even for relatively large CG segments. Following this, the CG method has gained momentum, and was adopted and generalized in several ways: (i) non-local hydrodynamics have been accounted for passive and active filaments in 2D, including wall interactions [27][28][29], (ii) 3D filament deformations were accounted for in [30,31], though limited to a local hydrodynamic resistive force theory (RFT), as in [12], (iii) it has been applied to study sperm flagellum propulsion in 2D [32], (iv) expanded into a hybrid immersed boundary method [33], as well as a stochastic method [34], and (v) used for analytical and numerical study of the well-posedness of Newtonian and viscoelastic elastohydrodynamic propulsion [35,36].…”
Section: Introductionmentioning
confidence: 99%