File:Propagating-Cell-Membrane-Waves-Driven-by-Curved-Activators-of-Actin-Polymerization-pone.0018635.s006.ogv
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Propagating-Cell-Membrane-Waves-Driven-by-Curved-Activators-of-Actin-Polymerization-pone.0018635.s006.ogv (Ogg Theora video file, length 1 min 7 s, 560 × 420 pixels, 182 kbps, file size: 1.45 MB)
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[edit]DescriptionPropagating-Cell-Membrane-Waves-Driven-by-Curved-Activators-of-Actin-Polymerization-pone.0018635.s006.ogv |
English: Simulation of solitary propagating structure that arose within our model when we removed the effects of the non-linear tension (), using the same values for the parameters as used for the calculation shown in Fig. 4B–D (diffusion(-)–adsorption(+). In this calculation we used the full expression for the exponential form of the adsorption of given in Eq.S6. Note that the membrane amplitude is clearly beyond the validity of the Monge representation of the membrane curvature. In this simulation we find that the CDR has a central bump where the convex activators are localized, while the concave activators form displaced bands at the front and the back. |
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Source | Movie S5 from Peleg B, Disanza A, Scita G, Gov N (2011). "Propagating Cell-Membrane Waves Driven by Curved Activators of Actin Polymerization". PLOS ONE. DOI:10.1371/journal.pone.0018635. PMID 21533032. PMC: 3080874. | ||
Author | Peleg B, Disanza A, Scita G, Gov N | ||
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Date/Time | Thumbnail | Dimensions | User | Comment | |
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current | 02:56, 14 November 2012 | 1 min 7 s, 560 × 420 (1.45 MB) | Open Access Media Importer Bot (talk | contribs) | Automatically uploaded media file from Open Access source. Please report problems or suggestions here. |
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Author | Peleg B, Disanza A, Scita G, Gov N |
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Usage terms | http://creativecommons.org/licenses/by/3.0/ |
Image title | Simulation of solitary propagating structure that arose within our model when we removed the effects of the non-linear tension (), using the same values for the parameters as used for the calculation shown in Fig. 4B?D (diffusion(-)?adsorption(+). In this calculation we used the full expression for the exponential form of the adsorption of given in Eq.S6. Note that the membrane amplitude is clearly beyond the validity of the Monge representation of the membrane curvature. In this simulation we find that the CDR has a central bump where the convex activators are localized, while the concave activators form displaced bands at the front and the back. |
Software used | Xiph.Org libtheora 1.1 20090822 (Thusnelda) |
Date and time of digitizing | 2011 |