{"title":"Active droplet driven by collective chemotaxis.","authors":"Christian Carlsson, Tong Gao","doi":"10.1039/d4sm00717d","DOIUrl":null,"url":null,"abstract":"<p><p>Surfactant-laden fluid interfaces of soft colloids, such as bubbles and droplets, are ubiquitously seen in various natural phenomena and industrial settings. In canonical systems where microparticles are driven in hydrodynamic flows, convection of the surfactant changes local surface tension. Subsequently, the interplay of Marangoni and hydrodynamic stresses leads to rich interfacial dynamics that directly impact the particle motions. Here we introduce a new mechanism for self-propelled droplets, driven by a thin layer of chemically active microparticles situated at the interface of a suspended droplet, which is a direct extension of the planar collective surfing model by Masoud and Shelley (H. Masoud and M. J. Shelley, <i>Phys. Rev. Lett.</i>, 2014, <b>112</b>, 128304). These particles can generate chemicals locally, leading to spontaneous Marangoni flows that drive the self-aggregation of microparticles. This process, in turn, creates a polarized surfactant distribution, which induces collective chemotaxis and dipolar bulk flows, ultimately breaking the symmetry. By assuming the local surfactant production to be either proportional to particle density or saturated at a high particle density, we observe that the system can be chemotactically diverging or approach a steady state with constant migration velocity. The system is studied analytically in the linear region for the initial transient dynamics, yielding critical numbers and familiar patterns, as well as numerically for larger amplitudes and over a long time using spectral methods.</p>","PeriodicalId":103,"journal":{"name":"Soft Matter","volume":" ","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2024-11-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Soft Matter","FirstCategoryId":"92","ListUrlMain":"https://doi.org/10.1039/d4sm00717d","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Surfactant-laden fluid interfaces of soft colloids, such as bubbles and droplets, are ubiquitously seen in various natural phenomena and industrial settings. In canonical systems where microparticles are driven in hydrodynamic flows, convection of the surfactant changes local surface tension. Subsequently, the interplay of Marangoni and hydrodynamic stresses leads to rich interfacial dynamics that directly impact the particle motions. Here we introduce a new mechanism for self-propelled droplets, driven by a thin layer of chemically active microparticles situated at the interface of a suspended droplet, which is a direct extension of the planar collective surfing model by Masoud and Shelley (H. Masoud and M. J. Shelley, Phys. Rev. Lett., 2014, 112, 128304). These particles can generate chemicals locally, leading to spontaneous Marangoni flows that drive the self-aggregation of microparticles. This process, in turn, creates a polarized surfactant distribution, which induces collective chemotaxis and dipolar bulk flows, ultimately breaking the symmetry. By assuming the local surfactant production to be either proportional to particle density or saturated at a high particle density, we observe that the system can be chemotactically diverging or approach a steady state with constant migration velocity. The system is studied analytically in the linear region for the initial transient dynamics, yielding critical numbers and familiar patterns, as well as numerically for larger amplitudes and over a long time using spectral methods.
在各种自然现象和工业环境中,经常可以看到充满表面活性剂的软胶体流体界面,如气泡和液滴。在典型的系统中,微颗粒在流体动力流中被驱动,表面活性剂的对流会改变局部表面张力。随后,马兰戈尼应力和流体动力应力的相互作用导致丰富的界面动力学,直接影响粒子的运动。在此,我们引入了一种新的液滴自推进机制,它由位于悬浮液滴界面上的一薄层化学活性微颗粒驱动,是 Masoud 和 Shelley(H. Masoud 和 M. J. Shelley,Phys.)这些微粒能在局部产生化学物质,导致自发的马兰戈尼流,推动微粒的自我聚集。这一过程反过来又会产生极化的表面活性剂分布,从而诱发集体趋化和双极体流,最终打破对称性。通过假设局部表面活性剂的产生与颗粒密度成正比或在颗粒密度较高时达到饱和,我们观察到系统可以趋化发散或以恒定的迁移速度接近稳定状态。我们在线性区域对该系统的初始瞬态动力学进行了分析研究,得出了临界值和熟悉的模式,并使用光谱方法对较大振幅和较长时间的瞬态动力学进行了数值研究。