2019
DOI: 10.1109/lcsys.2019.2919751
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Optimal Motion of a Scallop: Some Case Studies

Abstract: In this paper we focus on a two-link swimmer called scallop which moves changing dynamics between two fluids regimes. We address and solve explicitly two optimal control problems, the minimum time one and the minimum quadratic cost needed to move the swimmer between two fixed positions using a periodic control. Considering only one switching in the dynamics and exploiting the structure of the equation of motion we are able to split the problem into simpler ones. We solve explicitly each sub-problem obtaining a… Show more

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Cited by 7 publications
(4 citation statements)
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“…In consequence, the slow motion caused by a relatively small but long-lasting force is more effective than the fast one. The effect is similar to the slow-open, fast-close actuation mechanism of the scallop motion, the molecular motors-driven internal sliding of polymeric filaments in singly flagellated eukaryotes [57,58]; however, instead of the inertia or viscous effects being the cause of scallop or eukaryote motion, the motion of the analyzed copolymer is due to its energetic asymmetry. The forces exerted by part P2 on P1 of the chain computed as partial derivatives of the free Helmholtz energy (Figure 17) and averaged for positions of the chain mass center are collected in Figure 19.…”
Section: Mechanism Of Unidirectional Motionmentioning
confidence: 66%
“…In consequence, the slow motion caused by a relatively small but long-lasting force is more effective than the fast one. The effect is similar to the slow-open, fast-close actuation mechanism of the scallop motion, the molecular motors-driven internal sliding of polymeric filaments in singly flagellated eukaryotes [57,58]; however, instead of the inertia or viscous effects being the cause of scallop or eukaryote motion, the motion of the analyzed copolymer is due to its energetic asymmetry. The forces exerted by part P2 on P1 of the chain computed as partial derivatives of the free Helmholtz energy (Figure 17) and averaged for positions of the chain mass center are collected in Figure 19.…”
Section: Mechanism Of Unidirectional Motionmentioning
confidence: 66%
“…The minimal time optimal control problem seeks the optimal solution to move from a given configuration to another given one in the shortest possible time, whereas optimisation of the power expended deals with minimising the power expended to achieve the motion (this is useful in view in presence of limited amount of resources). Similar optimal control problems have been tackled in [7,9,19] for the power expended of a filament moving on a plane, for the minimal time of a planar Purcell swimmer, and for the minimal time ad quadratic cost for a scallop subject to a switching dynamics, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…The minimal time optimal control problem seeks the optimal solution to move from a given configuration to another given one in the shortest possible time, whereas optimization of the power expended deals with minimizing the power expended to achieve the motion (this is useful in consideration of a limited amount of resources). Similar optimal control problems have been tackled in [ 9 , 13 , 17 , 30 , 32 ] for the power expended of a filament moving on a plane, for the minimal time of a planar Purcell swimmer, and for the minimal time ad quadratic cost for a scallop subject to a switching dynamics, respectively.…”
Section: Introductionmentioning
confidence: 99%