scholarly journals Self-propelled swimming of a flexible filament driven by coupled plunging and pitching motions

2021 ◽  
Vol 33 (1) ◽  
pp. 157-169
Author(s):  
Bing-lin Li ◽  
Yi-wei Wang ◽  
Bo Yin ◽  
Xiang Zhang ◽  
Xing Zhang
Keyword(s):  
2014 ◽  
Vol 141 (17) ◽  
pp. 174904 ◽  
Author(s):  
Luis Cajamarca ◽  
Gregory M. Grason
Keyword(s):  

2018 ◽  
Vol 83 ◽  
pp. 40-53 ◽  
Author(s):  
Xingjian Lin ◽  
Guoyi He ◽  
Xinyi He ◽  
Qi Wang

Anales AFA ◽  
2018 ◽  
Vol 29 (1) ◽  
pp. 29-32
Author(s):  
G. van der Velde ◽  
C. Gómez ◽  
M. Freytes ◽  
L. Bruno ◽  
M.V. D’Angelo

Author(s):  
M. A. Korotkevich ◽  
N. V. Prokofieva

It is found that the voltage at the lowest points of the wire or cable sag and at the points of their suspension on the pillars in the same span, determined in accordance with the properties of a perfectly flexible filament (similar to which the wires and cables are located in the span), differ slightly, and taking the difference of the mentioned values into account is only of methodologycal importance. The article presents the results of the calculation of wire and cable sag of large spans of power transmission line of 500 m or more length using both the traditional theory of the catenary line and the theory of equal resistance, when the cross-sectional area of a wire or cable, proportional to their tension, is considered variable in the span length, which provides the same probability of breaking them at any point of the span. When calculating the wires and cables in normal and emergency conditions, the largest sags are determined, which take place either at a higher ambient temperature or at a load of the wire with ice. The wire must be mounted in such a way as to ensure the normalized permissible dimensions to crossed engineering structures, water barriers or land, that are determined depending on the nominal voltage of the line. It is noted that the values of the wire and cable sags determined using the theory of the catenary line for the transition spans are less (although slightly) as compared to the data obtained on the basis of the theory of the equal resistance circuit. This must be taken into account in the design process.


Author(s):  
Preethi L. Chandran ◽  
Mohammad R. K. Mofrad

In this paper we simulate the effect of hydrodynamic interaction on the Brownian dynamics of semiflexible filaments. Semiflexible filaments are those whose entropy-driven bending fluctuations are resisted by the elastic bending stiffness. Semiflexible filaments make up the structural scaffold of cell and tissue matrix, and understanding their dynamic behavior is necessary for studying force transmission and remodeling in cells and tissue matrix. Hydrodynamic interaction refers to force on filament mediated through the local solvent flow around it. The local solvent flow is induced by the motion of the filament itself. Dynamic studies of semiflexible filaments tend to assume a uniform friction coefficient at every point on the filament. However Lagamarsino et al [1] showed that even for a filament in uniform translation, most of the drag is localized at the filament ends, which increases the tendency of the filament to bend and rotate even under a uniform driving force. In this paper we explore how the combined effect of non-uniform friction coefficient due to hydrodynamic screening and the non-uniform local solvent flow due to the filament fluctuations affects its Brownian dynamics.


2014 ◽  
Vol 349 ◽  
pp. 1-11 ◽  
Author(s):  
Tai-Hsien Wu ◽  
Rurng-Sheng Guo ◽  
Guo-Wei He ◽  
Ying-Ming Liu ◽  
Dewei Qi

2019 ◽  
Vol 4 (7) ◽  
pp. 1900176 ◽  
Author(s):  
Abiodun Komolafe ◽  
Russel Torah ◽  
Yang Wei ◽  
Helga Nunes‐Matos ◽  
Menglong Li ◽  
...  
Keyword(s):  

2021 ◽  
Vol 930 ◽  
Author(s):  
Puja Sunil ◽  
Sanjay Kumar ◽  
Kamal Poddar

Experimental studies are conducted on a rotationally oscillating cylinder with an attached flexible filament at a Reynolds number of 150. Parametric studies are carried out to investigate the effect of cylinder forcing parameters and filament stiffness on the resultant wake structure. The diagnostics are flow visualization using the laser-induced fluorescence technique, frequency measurement using a hot film, and characterization of the velocity and vorticity field using planar particle image velocimetry. The streamwise force and power are estimated through control volume analysis, using a modified formulation, which considers the streamwise and transverse velocity fluctuations in the wake. These terms become important in a flow field where asymmetric wakes are observed. An attached filament significantly modifies the flow past a rotationally oscillating cylinder from a Bénard–Kármán vortex street to a reverse Bénard–Kármán vortex street, albeit over a certain range of Strouhal number, $St_{A} \sim 0.25\text {--}0.5$ , encountered in nature in flapping flight/fish locomotion and in the flow past pitching airfoils. The transition from a Kármán vortex street to a reverse Kármán vortex street precedes the drag-to-thrust transition. The mechanism of unsteady thrust generation is discussed. Maximum thrust is generated at the instants when vortices are shed in the wake from the filament tip. At $St_{A} > 0.4$ , a deflected wake associated with the shedding of an asymmetric vortex street is observed. Filament flexibility delays the formation of an asymmetric wake. Wake symmetry is governed by the time instant at which a vortex pair is shed in the wake from the filament tip.


2011 ◽  
Vol 84 (6) ◽  
Author(s):  
H. Ait Abderrahmane ◽  
M. P. Paidoussis ◽  
M. Fayed ◽  
H. D. Ng
Keyword(s):  

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