Fig. 2: Short- and long-time dynamics of the aggregates. | Nature Physics

Fig. 2: Short- and long-time dynamics of the aggregates.

From: Unconventional colloidal aggregation in chiral bacterial baths

Fig. 2

Short-time dynamics of the aggregates (Δt < 5 s): a, Inset: mean squared displacement for fixed bacterial concentration ρB = ρ* and increasing aggregate size RG (larger symbols for larger RG). The mean squared displacement increased linearly with time, with an effective diffusivity Deff(ρB,RG). a, Translational diffusivity Deff for various bacterial concentrations ρB and aggregate sizes RG (black is thermal and hotter colours represent higher ρB). Dashed lines are the Stokes–Einstein predictions Deff = α(ρB)/RG. Data symbols with error bars represent the average and standard deviation for more than five aggregates. b, Inset: mean squared angular displacement for fixed bacterial concentration ρB = ρ* and increasing aggregate size RG (larger symbols for larger RG). The mean squared angular displacement increased linearly with time, with an effective diffusivity \({D}_{{{{\rm{eff}}}}}^{\theta }({\rho }_\mathrm{B},{R}_\mathrm{G})\). b, Rotational diffusivity \({D}_{{{{\rm{eff}}}}}^{\theta }\) for various bacterial concentrations ρB and aggregate sizes RG (black is thermal and hotter colours represent higher ρB). Dashed lines are the Stokes–Einstein predictions \({D}_{{{{\rm{eff}}}}}^{\theta }=\beta ({\rho }_\mathrm{B})/{R}_\mathrm{G}^{3}\). Data symbols with error bars represent the average and standard deviation for more than five aggregates. c, Normalized diffusivity for translations α/α0 (circles) and rotations β/β0 (diamonds), where subscript 0 refers to the thermal bath. The normalized translational and rotational diffusivity collapsed. The symbols are slightly offset on the horizontal axis for clarity and represent the average and standard deviation (error bars). Long-time dynamics of the aggregates: d, Persistent clockwise rotation of aggregates observed at longer times (minutes to tens of minutes) in the glass capillary. The linear dependence of the angle θ (defined as in the inset) allowed us to extract a rotation rate Ω(ρB,RG). eh, Histograms of rotation rates Ω for different bacterial concentrations ρB for all aggregate sizes RG: ρB = ρ* (e); ρB = 0.5 ρ* (f); ρB = 0.2 ρ* (g); ρB = 0, thermal (h). i, Inset: rotation rates Ω for different bacterial concentrations (ρB ≈ 0.2 ρ* (green), ρB ≈ 0.5 ρ* (orange) and ρB ≈ ρ* (red), with ρ* = 6 x 108 cells per millilitre) and aggregate sizes RG. i, Data collapsed onto the master curve \({{\varOmega }}/({{{\mathcal{M}}}}{\rho }_\mathrm{B}) \propto 1/{R}_\mathrm{G}^{3}\), where \({{{\mathcal{M}}}}\) is the mass of an aggregate particle. Each point represents a measurement of an aggregate particle.

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