2013
DOI: 10.1103/physreve.87.010901
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Spontaneous motion of an elliptic camphor particle

Abstract: The coupling between deformation and motion in a self-propelled system has attracted broader interest. In the present study, we consider an elliptic camphor particle for investigating the effect of particle shape on spontaneous motion. It is concluded that the symmetric spatial distribution of camphor molecules at the water surface becomes unstable first in the direction of a short axis, which induces the camphor disk motion in this direction. Experimental results also support the theoretical analysis. From th… Show more

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Cited by 38 publications
(49 citation statements)
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References 28 publications
(28 reference statements)
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“…The mass m is set to 0.01. resistance coefficient were numerically obtained based on Eqs. (18) and (19). The stable and unstable amplitudes were obtained by numerical calculations performed in forward and backward time directions, respectively.…”
Section: (C3)mentioning
confidence: 99%
“…The mass m is set to 0.01. resistance coefficient were numerically obtained based on Eqs. (18) and (19). The stable and unstable amplitudes were obtained by numerical calculations performed in forward and backward time directions, respectively.…”
Section: (C3)mentioning
confidence: 99%
“…Similarly, a leading order approximation to the boundary layer flow profile driven by the surfactant whose dynamics are dominated by the dissolved phase [20] is Our result is quite robust, as we demonstrated for two surfactants varying in their CMC values by factor 100, and can be used with other surfactants. We used these signatures to determine that CA released from a gel tablet spreads in an adsorbed phase, a result that bears upon Marangoni-driven self-assembly [27][28][29][30][31][32] and propulsion [33][34][35][36]. Assumptions about surfactant dynamics, such as made in Ref.…”
Section: Signaturementioning
confidence: 99%
“…In particular, droplet shape deformations are not negligible, since the coupling between the shape and motion plays an important role in the self-motion of the droplet as has been reported in previous works. 17,18,[20][21][22][23][24][25] Several studies have already been made for the modeling of a deformable self-propelled droplet. [26][27][28][29][30][31][32][33] However, in the case of multiple droplets, the individual volumes are not precisely maintained in these models; hence the droplets exchange mass.…”
Section: Introductionmentioning
confidence: 99%