2020
DOI: 10.1103/physrevlett.125.018003
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Symmetric Mixtures of Pusher and Puller Microswimmers Behave as Noninteracting Suspensions

Abstract: Suspensions of rear-and front-actuated microswimmers immersed in a fluid, known respectively as "pushers" and "pullers," display qualitatively different collective behaviors: beyond a characteristic density, pusher suspensions exhibit a hydrodynamic instability leading to collective motion known as active turbulence, a phenomenon which is absent for pullers. In this Letter, we describe the collective dynamics of a binary pusher-puller mixture using kinetic theory and large-scale particle-resolved simulations. … Show more

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Cited by 22 publications
(17 citation statements)
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References 49 publications
(90 reference statements)
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“…28 × 10 −8 kg/s is the calculated drag coefficient of bacterial body orientated along its major axis, which is slightly smaller than the measured value shown above. The linear stability analysis of the original kinetic theories can be easily extended for the mixture of mobile and immobile bacteria (14,44), which results in f as the prefactor of v in Eq. 2.…”
Section: D Phase Diagrammentioning
confidence: 99%
“…28 × 10 −8 kg/s is the calculated drag coefficient of bacterial body orientated along its major axis, which is slightly smaller than the measured value shown above. The linear stability analysis of the original kinetic theories can be easily extended for the mixture of mobile and immobile bacteria (14,44), which results in f as the prefactor of v in Eq. 2.…”
Section: D Phase Diagrammentioning
confidence: 99%
“…There has been considerable work examining the interactions of other kinds of microswimmers, e.g., phoretic particles [46], active droplets [26], active particles [10] and mixed suspensions [47]. However, in addition to hydrodynamic interactions, chemical trails can be far-reaching, and therefore affect the far-field dynamics.…”
Section: Discussionmentioning
confidence: 99%
“…These can in turn be related to physical units by rescaling with the corresponding dipole lengths and swimming speeds of the experimental system in question: for E. coli, l ≈ 2 µm, v s ≈ 20 µm/s, and F ≈ 0.4 pN [7]. The model introduced in the previous Section has been extensively used to study the onset of collective motion in dilute suspensions of pusher-like microswimmers [35,39,49], and its phenomenology is wellunderstood. Below the threshold value n c of the number density n = N/V of microswimmers, the suspension remains homogeneous and isotropic while exhibiting significant correlations between microswimmers.…”
Section: Model and Methodsmentioning
confidence: 99%