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. 2021 Dec 6;12:7088. doi: 10.1038/s41467-021-26942-0

Fig. 4. Polymer trajectories and distributions for the trapping time and hop length.

Fig. 4

a Representative (1D) displacements, Δxc(t), of polymers with different reversal rates, λ, as a function of time for Pe = 50. Horizontal solid lines indicate the trapping phases for different λ. (Inset) Particle trajectories of the center monomer of a rarely reversing polymer, λτ0 = 5 · 10−4 (black ; magnified by a factor of 4), and moderately reversing polymers, λτ0 = 0.5 and 15 (blue and red, respectively). The trajectories are shown in the xy plane, (Δxc(t), Δyc(t)). b Trapping time distribution φT(t) and c hop length distribution φH() for Pe = 50 and different reversal rates, λ, extracted from individual trajectories. The inset in b shows the fraction of time spent hopping p = τH/(τH + τT) and the average trapping time τT/τ0 as a function of λτ0. The black solid line in panel c indicates the chord length distribution of the medium φLc(). The inset in c shows the average hopping length 〈H〉 normalized by the average chord length 〈Lc〉 of the porous medium. Source data are provided as a Source Data file.