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. Author manuscript; available in PMC: 2014 Dec 1.
Published in final edited form as: Nat Mater. 2014 May 4;13(6):631–637. doi: 10.1038/nmat3960

Figure 3. Integrin-FN clutch model of force transmission.

Figure 3

(a) Myosin motors pull on actin filaments, which move with rearward speed va. Integrins of two different types connect to the actin flow through adaptor proteins, and compete for binding to FN with effective binding rates kon1 and kon2 given by true binding rates (kont1, kont2) multiplied by integrin densities on the membrane (dint1, dint2). FN molecules are in turn connected to a compliant substrate, represented as a linear elastic spring of varying rigidity. (b) Flow of events (from top to bottom). (i) The model considers a given number of FN molecules (triangles) attached to the substrate, to which integrins can bind. (ii) Orange integrins, with higher kon, will bind faster. (iii) Once they bind, actin rearward movement applies a force on all integrins and the substrate. Because orange integrins also have a higher koff, they will detach sooner. (iv) Eventually, blue integrins will detach as well, and if before detaching the force transmitted through them reaches a threshold value, a reinforcement mechanosensing event will result in increased integrin density. (v) Once all integrins detach, force on the substrate is released and the cycle begins again. (c-e) Cell traction forces (c), integrin densities (d), and actin speeds (e) predicted by the model, the three regimes (1-3) are discussed in the main text and in Supplementary Note 4.