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. 2021 Mar 4;82(4):28. doi: 10.1007/s00285-021-01550-0

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© The Author(s) 2021

Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

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Fig. 14 — Simulations of the combined model (CM), where only the profiles of u are shown. The profiles of v show mostly similar patterns. Parameters as in Table 4 (CM2) but varying s, and HSS+noise initial condition as described in the text. As we increase the actin feedback strength s, the behavior transitions from slowly moving, repelling peaks to colliding peaks. At higher s, there is a rapidly oscillating standing wave pattern in some parts of the domain