Volume 111, Issue 8, Pages (October 2016)

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Volume 111, Issue 8, Pages 1589-1592 (October 2016) Theory from the Oster Laboratory Leaps Ahead of Experiment in Understanding Actin- Based Cellular Motility  Thomas D. Pollard  Biophysical Journal  Volume 111, Issue 8, Pages 1589-1592 (October 2016) DOI: 10.1016/j.bpj.2016.08.044 Copyright © 2016 Biophysical Society Terms and Conditions

Figure 1 Actin filaments in motile keratocytes. (left) Superimposed series of phase contrast micrographs at 15 s intervals of fish keratocytes moving on a glass slide. (middle) Fluorescence micrograph of a cell stained with rhodamine-phalloidin to label actin filaments. (right) Transmission electron micrograph of the leading edge of a cell fixed while moving to the right and prepared by extraction, critical point drying and shadowing with platinum. (Courtesy of Gary Borisy and Tanya Svitkina). To see this figure in color, go online. Biophysical Journal 2016 111, 1589-1592DOI: (10.1016/j.bpj.2016.08.044) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 2 Brownian ratchet model from Peskin et al. (12). Diffusive fluctuations in the position of the barrier (D) open up space for insertion of an actin subunit at the end of the filament. The graph shows the dependence of the velocity on load on the barrier at 10 μM actin monomers. The continuous and dashed lines are the results using two different sets of assumptions (12). Biophysical Journal 2016 111, 1589-1592DOI: (10.1016/j.bpj.2016.08.044) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 3 Elastic Brownian ratchet model from Mogilner and Oster (13) showing an orthogonal network of flexible actin filaments fluctuating as they grow near the inside of the plasma membrane. The optimal angle (θ) for transducing polymerization into displacement of the membrane is ∼50°. Biophysical Journal 2016 111, 1589-1592DOI: (10.1016/j.bpj.2016.08.044) Copyright © 2016 Biophysical Society Terms and Conditions

Figure 4 Dendritic nucleation model from Pollard and Borisy (21). Note the 70° branches formed by Arp2/3 complex, fluctuating filaments pushing at an angle against the inside of the plasma membrane as they elongate, and capping to keep the lengths of the branches short enough to push effectively. (Reproduced with permission from Cell). To see this figure in color, go online. Biophysical Journal 2016 111, 1589-1592DOI: (10.1016/j.bpj.2016.08.044) Copyright © 2016 Biophysical Society Terms and Conditions