2018
DOI: 10.1039/c8sm00690c
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Clustering-induced self-propulsion of isotropic autophoretic particles

Abstract: Isotropic phoretic particles do not swim individually but can achieve self-propulsion collectively by spontaneously forming clusters of anisotropic geometry.

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Cited by 67 publications
(93 citation statements)
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References 64 publications
(102 reference statements)
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“…In the following, the general framework is first presented for the chemical problem, generalizing the method proposed in [77] for homogeneous particles to the general case of arbitrary surface activity, in order to determine the successive moments of the surface concentration on each particle as a result of their activity. In a second step, the corresponding method is presented for the hydrodynamic problem using the output of the chemical dynamics as a forcing and constructing the resulting particle velocities.…”
Section: The Methods Of Reflections For Phoretic Problemsmentioning
confidence: 99%
See 1 more Smart Citation
“…In the following, the general framework is first presented for the chemical problem, generalizing the method proposed in [77] for homogeneous particles to the general case of arbitrary surface activity, in order to determine the successive moments of the surface concentration on each particle as a result of their activity. In a second step, the corresponding method is presented for the hydrodynamic problem using the output of the chemical dynamics as a forcing and constructing the resulting particle velocities.…”
Section: The Methods Of Reflections For Phoretic Problemsmentioning
confidence: 99%
“…In this highly-symmetric setting, the chemical and hydrodynamic fields as well as the particles' velocities can be obtained analytically for an arbitrary distance using bispherical coordinates [66,77] (Appendix B). The resulting flow and concentration fields are reported on Figure 5.…”
Section: A Axisymmmetric Relative Translation Of Two Janus Particlesmentioning
confidence: 99%
“…In this system, long-ranged attractive and short-ranged repulsive drift velocities are generated by a balance between attraction due to chemotaxis and repulsion due to phoresis. This can be contrasted with other propelling clusters where the symmetry is broken by the shape of the cluster [37,38,53,58]. For two identical attractive swimmers, the condition to form a stationary dimer is V(0, 0, R 0 )=0, as seen in figure 9(a).…”
Section: Active Dimersmentioning
confidence: 99%
“…As active particles function under a sustained energy input within an ambient medium, their effective pair interactions are in general non-reciprocal and can systematically draw both linear and angular momentum from their surroundings. The roles of hydrodynamic flow [18][19][20][21][22][23][24], diffused solute [25][26][27][28][29], local phase change [30] and optical shadowing [31,32] as mediators of these interactions have been studied, as well as guidance by nearby boundaries [33][34][35]. Unravelling the dependence of phoretic and chemotactic effects on the surface profiles of catalyst concentration and solute-colloid interaction [8,[36][37][38] and symmetry-based classifications of pair interactions [39] have opened up the possibility of engineering active colloids with desired behaviour [40,41].…”
Section: Introductionmentioning
confidence: 99%
“…As one of their main characteristics, these systems are intrinsically out of equilibrium allowing them to self-organize into new ordered and even functional structures. In synthetic active systems, such structures include dynamic clusters which dynamically form and break-up in low density Janus colloids [4][5][6][7][8] as well as laser driven colloids which spontaneously start to move ballistically (self-propel) when binding together [9][10][11]. Likewise, biological microswimmers form patterns such as vortices in bacterial turbulence [12][13][14][15], or swirls and microflock patterns in chiral active matter like curved polymers or sperm [16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%