2017
DOI: 10.1103/physreve.95.023108
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Scale-dependent colocalization in a population of gyrotactic swimmers

Abstract: We study the small scale clustering of gyrotactic swimmers transported by a turbulent flow, when the intrinsic variability of the swimming parameters within the population is considered. By means of extensive numerical simulations, we find that the variety of the population introduces a characteristic scale R * in its spatial distribution. At scales smaller than R * the swimmers are homogeneously distributed, while at larger scales an inhomogeneous distribution is observed with a fractal dimension close to wha… Show more

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Cited by 3 publications
(11 citation statements)
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References 32 publications
(59 reference statements)
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“…A similar argument can be done for swimmers with the same stability parameter and different swimming velocities where one finds R * ηΨ∆Φ [92]. For R < R * the separation dynamics is dominated by the parameter mismatch and one expect poor correlation between the swimmers, i.e.…”
Section: Clustering Of Polydisperse Populationssupporting
confidence: 52%
See 1 more Smart Citation
“…A similar argument can be done for swimmers with the same stability parameter and different swimming velocities where one finds R * ηΨ∆Φ [92]. For R < R * the separation dynamics is dominated by the parameter mismatch and one expect poor correlation between the swimmers, i.e.…”
Section: Clustering Of Polydisperse Populationssupporting
confidence: 52%
“…below the Kolmogorov length η, the velocity field is smooth and we can write ∆u(R) ∼ u η (R/η). Thus from the balance of the two terms in the above equation a characteristic scale emerges [92]:…”
Section: Clustering Of Polydisperse Populationsmentioning
confidence: 99%
“…Additionally, the condition v eff < v max defines a region in the {v s , α} parameter space for which swimmers are trapped. For the Lamb-Oseen vortex we numerically obtain v max ≈ 0.726 as the maximum of (16). Hence, by taking into account the role of shape, microswimmers with much lower swimming velocity v s than the maximum fluid velocity u 0 can escape the vortex.…”
Section: Fixed-point Analysismentioning
confidence: 79%
“…To elucidate this, we begin by considering spherical swimmers (α = 0). It is well known that, in general, equations for spherical swimmers following (1) and (2) conserve phasespace volume [11,16,21] ∇ x ·ẋ + ∇p ·ṗ = 0.…”
Section: Distributionsmentioning
confidence: 99%
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