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. 2011 Nov 28;195(5):799–813. doi: 10.1083/jcb.201101055

Figure 9.

Figure 9.

A physical model for contractile ring dynamics. (A) Full scalability based on contractile unit hypothesis (ϕ = 1, λ = 0). (B) Super scalability due to scalable initial myosin density only (ϕ0 = 1, ζ = 0.5, λ = 0). (C) Size-dependent actin turnover leads to either full scalability (solid lines, ϕ0 = 1, ζ = 0) or super scalability (dashed lines, ϕ0 = 1, ζ > 0). (D) Size-independent actin turnover leads to partial scalability, as shown in experimental N. crassa data (symbols). Model (lines) uses fitted parameters (ζ = 0.3 ± 0.05, ϕ0 = 0.00085 ± 0.00015 s−1 [including uncertainty estimates], and λ = 0.052 ± 0.012 µm/s).