4.4 Article

Role of Marangoni forces in the velocity of symmetric interfacial swimmers

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PHYSICAL REVIEW FLUIDS
卷 6, 期 10, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevFluids.6.104006

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  1. French research programs [ANR-16-CE30-0028]
  2. University of Lyon in the framework of the French program Programme Investissements d'Avenir [ANR-16-IDEX-0005]
  3. Agence Nationale de la Recherche (ANR) [ANR-16-CE30-0028] Funding Source: Agence Nationale de la Recherche (ANR)

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The research focuses on interfacial swimmers that propel themselves by releasing surfactants, with a key role played by Marangoni effects. Low Pe* regime shows bistability with threshold Marangoni number, while high Pe* regime features a robust scaling law with exponent close to 3/4.
Interfacial swimmers are objects that self-propel at an interface by autonomously generating a gradient of surface tension, often through the continuous release of a surfactant. While the case of asymmetric swimmers has long been studied, experiments have shown that spontaneous motion is also possible for symmetric swimmers. The basic mechanism of symmetry-breaking is qualitatively well-established but one key aspect of the phenomenon that has proved particularly difficult to elucidate is the role of Marangoni effects in the self-propulsion. We address this question by numerical methods, which can fully handle the complex interplay between swimmer motion, fluid flow, surfactant distribution, and Marangoni stresses. Our swimmer is a disk releasing a soluble surfactant in a deep-layer fluid. We investigate how the swimming velocity, represented by a Peclet number Pe* depends on its characteristics, as encapsulated in the Marangoni number M. We analyze the properties of the swimming diagram Pe*(M) and compare with approximate models to understand their origin. We find that the low-Pe* regime exhibits a bistability region: spontaneous swimming involves a threshold Marangoni number, a discontinuity in velocity and possibly hysteresis. Those features are present only for a full description of the problem and reveal the subtle but key role of Marangoni flows. The large-Pe* regime features a robust asymptotic scaling law Pe* similar to M-alpha, whose exponent alpha similar or equal to 0.72 is close to the 3/4 value predicted by a simplified model, indicating a much weaker influence of Marangoni flows. While our results were obtained assuming a point-source swimmer in the Stokes flow regime, we show that the picture remains very similar when considering a spatially extended source size, finite Reynolds number, or a fixed concentration swimmer. We discuss our findings in relation to experiments.

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