FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W3011082908> ?p ?o ?g. }

• W3011082908 abstract "ABSTRACT The rhythmic motions and wave-like planar oscillations in filamentous soft structures are ubiquitous in biology. Inspired by these, recent work has focused on the creation of synthetic colloid-based active mimics that can be used to move, transport cargo, and generate fluid flows. Underlying the functionality of these mimics is the coupling between elasticity, geometry, dissipation due to the fluid, and active force or moment generated by the system. Here, we use slender body theory to analyze the linear stability of a subset of these - active elastic filaments, filament arrays and filament carpets - animated by follower forces. Follower forces can be external or internal forces that always act along the filament contour. The application of slender body theory enables the accurate inclusion of hydrodynamic effects, screening due to boundaries, and interactions between filaments. We first study the stability of fixed and freely suspended sphere-filament assemblies, calculate neutral stability curves separating stable oscillatory states from stable straight states, and quantify the frequency of emergent oscillations. When shadowing effects due to the physical presence of the spherical boundary are taken into account, the results from the slender body theory differ from that obtained using local resistivity theory. Next, we examine the onset of instabilities in a small cluster of filaments attached to a wall and examine how the critical force for onset of instability and the frequency of sustained oscillations depend on the number of filaments and the spacing between the filaments. Our results emphasize the role of hydrodynamic interactions in driving the system towards perfectly in-phase or perfectly out of phase responses depending on the nature of the instability. Specifically, the first bifurcation corresponds to filaments oscillating in-phase with each other. We then extend our analysis to filamentous (line) array and (square) carpets of filaments and investigate the variation of the critical parameters for the onset of oscillations and the frequency of oscillations on the inter-filament spacing. The square carpet also produces a uniform flow at infinity and we determine the ratio of the mean-squared flow at infinity to the energy input by active forces. We conclude by analyzing the bending and buckling instabilities of a straight passive filament attached to a wall and placed in a viscous stagnant flow - a problem related to the growth of biofilms, and also to mechanosensing in passive cilia and microvilli. Taken together, our results provide the foundation for more detailed non-linear analyses of spatiotemporal patterns in active filament systems." @default.
• W3011082908 created "2020-03-23" @default.
• W3011082908 creator A5007809664 @default.
• W3011082908 creator A5069452950 @default.
• W3011082908 date "2020-03-12" @default.
• W3011082908 modified "2023-10-16" @default.
• W3011082908 title "Elastohydrodynamical instabilities of active filaments, arrays and carpets analyzed using slender body theory" @default.
• W3011082908 cites W1973541870 @default.
• W3011082908 cites W1973632706 @default.
• W3011082908 cites W1989630959 @default.
• W3011082908 cites W1989813669 @default.
• W3011082908 cites W1994320812 @default.
• W3011082908 cites W1998479690 @default.
• W3011082908 cites W2001815952 @default.
• W3011082908 cites W2005402136 @default.
• W3011082908 cites W2008383218 @default.
• W3011082908 cites W2015775780 @default.
• W3011082908 cites W2017414316 @default.
• W3011082908 cites W2025562104 @default.
• W3011082908 cites W2028605946 @default.
• W3011082908 cites W2031167125 @default.
• W3011082908 cites W2032227660 @default.
• W3011082908 cites W2036312030 @default.
• W3011082908 cites W2049462154 @default.
• W3011082908 cites W2052788168 @default.
• W3011082908 cites W2056707942 @default.
• W3011082908 cites W2072618554 @default.
• W3011082908 cites W2075115399 @default.
• W3011082908 cites W2079566817 @default.
• W3011082908 cites W2080336455 @default.
• W3011082908 cites W2083922705 @default.
• W3011082908 cites W2087239777 @default.
• W3011082908 cites W2089680707 @default.
• W3011082908 cites W2119376602 @default.
• W3011082908 cites W2119763712 @default.
• W3011082908 cites W2130038980 @default.
• W3011082908 cites W2151970138 @default.
• W3011082908 cites W2158708699 @default.
• W3011082908 cites W2161355277 @default.
• W3011082908 cites W2286205318 @default.
• W3011082908 cites W2320560325 @default.
• W3011082908 cites W2328609331 @default.
• W3011082908 cites W2407515555 @default.
• W3011082908 cites W2499719923 @default.
• W3011082908 cites W2531276990 @default.
• W3011082908 cites W2544911403 @default.
• W3011082908 cites W2565287082 @default.
• W3011082908 cites W2586550673 @default.
• W3011082908 cites W2610854859 @default.
• W3011082908 cites W2734938303 @default.
• W3011082908 cites W2746196359 @default.
• W3011082908 cites W2747315297 @default.
• W3011082908 cites W2807294890 @default.
• W3011082908 cites W2807959585 @default.
• W3011082908 cites W2897909413 @default.
• W3011082908 cites W2932706456 @default.
• W3011082908 cites W2945037233 @default.
• W3011082908 cites W2963961277 @default.
• W3011082908 cites W2965604600 @default.
• W3011082908 cites W3099123631 @default.
• W3011082908 cites W3100885632 @default.
• W3011082908 cites W3102095090 @default.
• W3011082908 cites W4243898165 @default.
• W3011082908 cites W47671810 @default.
• W3011082908 doi "https://doi.org/10.1101/2020.03.10.986596" @default.
• W3011082908 hasPublicationYear "2020" @default.
• W3011082908 type Work @default.
• W3011082908 sameAs 3011082908 @default.
• W3011082908 citedByCount "3" @default.
• W3011082908 countsByYear W30110829082020 @default.
• W3011082908 crossrefType "posted-content" @default.
• W3011082908 hasAuthorship W3011082908A5007809664 @default.
• W3011082908 hasAuthorship W3011082908A5069452950 @default.
• W3011082908 hasBestOaLocation W30110829081 @default.
• W3011082908 hasConcept C121332964 @default.
• W3011082908 hasConcept C121684516 @default.
• W3011082908 hasConcept C121854251 @default.
• W3011082908 hasConcept C134306372 @default.
• W3011082908 hasConcept C134786449 @default.
• W3011082908 hasConcept C14228908 @default.
• W3011082908 hasConcept C159985019 @default.
• W3011082908 hasConcept C18762648 @default.
• W3011082908 hasConcept C192562407 @default.
• W3011082908 hasConcept C207821765 @default.
• W3011082908 hasConcept C33923547 @default.
• W3011082908 hasConcept C41008148 @default.
• W3011082908 hasConcept C57879066 @default.
• W3011082908 hasConcept C62354387 @default.
• W3011082908 hasConcept C74650414 @default.
• W3011082908 hasConcept C97355855 @default.
• W3011082908 hasConceptScore W3011082908C121332964 @default.
• W3011082908 hasConceptScore W3011082908C121684516 @default.
• W3011082908 hasConceptScore W3011082908C121854251 @default.
• W3011082908 hasConceptScore W3011082908C134306372 @default.
• W3011082908 hasConceptScore W3011082908C134786449 @default.
• W3011082908 hasConceptScore W3011082908C14228908 @default.
• W3011082908 hasConceptScore W3011082908C159985019 @default.
• W3011082908 hasConceptScore W3011082908C18762648 @default.
• W3011082908 hasConceptScore W3011082908C192562407 @default.
• W3011082908 hasConceptScore W3011082908C207821765 @default.

• next