Coherent locomotion as an attracting state for a free flapping body
Open accessAbstract
A recent experiment [Vandenberghe, N., Zhang, J. & Childress, S. (2004) J. Fluid Mech. 506, 147-155] has shown that an axle-mounted blade can spontaneously rotate when oscillated (or "flapped") above a critical frequency in a fluid. To understand the nature of flapping locomotion we study numerically the dynamics of a simple body, flapped up and down within a viscous fluid and free to move horizontally. We show here that, at sufficiently large "frequency Reynolds number," unidirectional locomotion emerges as an attracting state for an initially nonlocomoting body. Locomotion is generated in two stages: first, the fluid field loses symmetry by an instability similar to the classical von Kármán instability; and second, precipitous interactions with previously shed vortical structures "push" the body into locomotion. Body mass and slenderness play central and unexpected roles in each stage. Conceptually, this work demonstrates how locomotion can be transduced from the simple oscillations of a body through an interaction with its fluid environment.
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Flapping fins and undulatory swimming do not appear for Re_m < 10.
“Flapping fins and undulatory swimming do not appear for Re m < 10 [2, 5, 38].”
From Reynolds number limits for jet propulsion: a numerical study of simplified jellyfish (2011) · cites this paper as [2]
These vortical structures push the body into motion.
“These vortical structures push the body into motion.”
From Reynolds number limits for jet propulsion: a numerical study of simplified jellyfish (2011) · cites this paper as [2]
The fluid field loses symmetry when vortices formed behind the plate are alternately shed from each side.
“The fluid field loses symmetry when vortices formed behind the plate are alternately shed from each side.”
From Reynolds number limits for jet propulsion: a numerical study of simplified jellyfish (2011) · cites this paper as [2]
The transition from flapping to no flapping is connected to a change in the behavior of the vortex wake behind the flapping plate or appendage.
“Alben and Shelley [2] connect this transition to a change in the behavior of the vortex wake behind the flapping plate or appendage.”
From Reynolds number limits for jet propulsion: a numerical study of simplified jellyfish (2011) · cites this paper as [2]
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Reynolds number limits for jet propulsion: a numerical study of simplified jellyfish
Herschlag, G., & Miller, L. (2011) · Journal of Theoretical Biology · doi:10.1016/j.jtbi.2011.05.035 · Cited by 79 · see citing works
- Authors
- Alben, S., & Shelley, M.
- Affiliations
- Harvard University (US)
- Venue
- Proceedings of the National Academy of Sciences
- Publisher
- National Academy of Sciences
- Published
- 2005-07-29
- Volume
- 102
- Issue
- 32
- Pages
- 11163-11166
- ISSN
- 0027-8424 (ISSN-L)
- 1091-6490
- PMC
- PMC1183592
- OpenAlex
- W2020779850
- Cited by
- 179
- References
- 16
- Citations by year
- 2026: 6 · 2025: 8 · 2024: 8 · 2023: 5 · 2022: 8 · 2021: 11 · 2020: 10 · 2019: 10 · 2018: 11 · 2017: 10 · 2016: 9 · 2015: 18 · 2014: 12 · 2013: 8 · 2012: 11
- FWCI
- 9.26
- Type
- journal article
- Language
- en
- Open access
- green
- europepmc.org
- Locations
- Proceedings of the National Academy of Sciences (publishedVersion)
- Europe PMC (PubMed Central) (publishedVersion)
- PubMed Central (publishedVersion)
- PubMed (publishedVersion)
- Topics
- Physical Sciences › Engineering › Aerospace Engineering › Biomimetic flight and propulsion mechanisms
- Physical Sciences › Engineering › Computational Mechanics › Fluid Dynamics and Vibration Analysis
- Physical Sciences › Physics and Astronomy › Condensed Matter Physics › Micro and Nano Robotics
- Keywords
- flapping locomotion, spontaneous rotation, blade vibration, vortex structures, body mass, viscous fluid
- MeSH terms
- Animals, Biomechanical Phenomena, Computer Simulation, Flight, Animal, Models, Theoretical, Rheology
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