2021
DOI: 10.1017/jfm.2021.43
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Collective locomotion of two-dimensional lattices of flapping plates. Part 2. Lattice flows and propulsive efficiency

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Cited by 9 publications
(5 citation statements)
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“…Notable advancements have been made in comprehending oscillation-based principles and mechanisms. These advancements encompass a broad range of areas, including the optimisation of kinematics (Tuncer & Kaya 2005), exploration of three-dimensional effects (Dong, Mittal & Najjar 2006), manipulation of flow structures (Fish & Lauder 2006), investigation of flexibility influence (Zhu 2007; Alben 2008) as well as the study of multiple-foil configurations and collective arrangements (Muscutt, Weymouth & Ganapathisubramani 2017; Alben 2021). However, the existing studies on both the biological thrust generation and oscillating foil propulsion have been limited exclusively to homogeneous flows.…”
Section: Introductionmentioning
confidence: 99%
“…Notable advancements have been made in comprehending oscillation-based principles and mechanisms. These advancements encompass a broad range of areas, including the optimisation of kinematics (Tuncer & Kaya 2005), exploration of three-dimensional effects (Dong, Mittal & Najjar 2006), manipulation of flow structures (Fish & Lauder 2006), investigation of flexibility influence (Zhu 2007; Alben 2008) as well as the study of multiple-foil configurations and collective arrangements (Muscutt, Weymouth & Ganapathisubramani 2017; Alben 2021). However, the existing studies on both the biological thrust generation and oscillating foil propulsion have been limited exclusively to homogeneous flows.…”
Section: Introductionmentioning
confidence: 99%
“…Here, we use “mock flocks” or groups of self-propelling foils to investigate the structural and dynamical consequences of interactions through visco-inertial flows. We focus on linear formations in which many bodies are arranged serially or in tandem and whose dynamics within the formation are free and interactive 23 , 28 , 31 , 34 , 36 , 39 . Among all configurations, this setting is perhaps the most amenable to a detailed treatment of the flow-structure interactions, since the formation and dynamical freedom are one-dimensional (1D) and the flows quasi-2D.…”
Section: Introductionmentioning
confidence: 99%
“…Studies on flapping foils in side‐by‐side arrangements have demonstrated that the hydrodynamic thrust is relatively large when the foils flap in antiphase [12, 24]. Methods that solve the Navier–Stokes equations directly, such as the immersed boundary method [22, 33, 40] or marker‐and‐cell scheme [7, 8], require a fine computational grid near the bodies in order to resolve thin boundary layers and are thus limited to moderate Reynolds numbers, Re=O(102)O(103)${\textrm {Re}}=O(10^2)-O(10^3)$. Accurate and tractable simulations in regimes relevant to many swimming animals and biomimetic vehicles (e.g., Re=O(106)O(107)${\textrm {Re}}=O(10^6)-O(10^7)$ for dolphins [58]) have thus remained elusive.…”
Section: Introductionmentioning
confidence: 99%