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. 2014 Feb 4;106(3):526–534. doi: 10.1016/j.bpj.2013.12.031

Figure 1.

Figure 1

Creep response to uniaxial applied stress. (A) A schematic view of the simulated stress test. A cross-linked actin network is pinned at the –x boundary, and a stress (σ) is applied to the free +x boundary. (B) Snapshots of the deforming network at t = 0, 30, and 90 s with a relative filament turnover rate (n) = 0.1 and σ = 10 Pa. (C) Time evolution of network strain (ε) as a function of time for n = 0.1 and σ = 0.2 Pa (green dashed line); n = 0.1 and σ = 10 Pa (blue dotted line); and n = 0 and σ = 10 Pa (red solid line). (D) A strain rate (ε˙) as a function of σ for n = 0.1. (Inset) Effective viscosity (ηeff) as a function of σ. (E) Elastic (σe, open symbols) and viscous stress (σv, solid symbols) depending on σ at n = 0.1. (Inset) ηeff originating from σe (= σe/ε˙, open symbols) and σv (= σv/ε˙, solid symbols), respectively. Dashed lines in D and E indicate either ∼σ1 or ∼σ0. To see this figure in color, go online.