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. 2020 Oct 6;82(10):132. doi: 10.1007/s11538-020-00810-2

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© The Author(s) 2020

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 — Convergence study for a monolayer population consisting initially of 19 cells. The parameter $α$ of the GLS force was chosen independently of the spring stiffness $μ$ as $α = 7.51$ by fitting force intensities over the adhesive regime (strategy #1 in Sect. 3.2.1). The numerical solver used was (a) the forward Euler method, (b) the midpoint method and (c) the Adams–Bashforth method. The axes of the plots are in logarithmic scale. The dotted lines show a linear (plot (a)) and a quadratic function (plots (b) and (c)) to facilitate observation of the convergence order.