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      Correction to: Gyrotactic cluster formation of bottom-heavy squirmers

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          Abstract

          Correction to:The European Physical Journal E (2022) 45:1-14 10.1140/epje/s10189-022-00183-5 Equation (9) should read the balance between the angular velocities from the external bottom-heavy torque (Eq. (5)) and from the Stokeslet vorticity (Eq. (6)). However, a factor of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\frac{3}{4}$$\end{document} 3 4 was erroneously omitted. The corrected equation reads 9 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \frac{3}{4}\frac{{v_{0} }}{R}\frac{{r_{0} }}{R\alpha }\sin \vartheta = \frac{3}{4}\frac{{v_{0} }}{\alpha }\frac{R}{{r^{2} }}. $$\end{document} 3 4 v 0 R r 0 R α sin ϑ = 3 4 v 0 α R r 2 . Consequently, the two subsequent equations, where r = 2R, should read 10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \sin \vartheta = \frac{{1{/(4}\alpha {)}}}{{r_{0} {/(}R\alpha {)}}}. $$\end{document} sin ϑ = 1 / ( 4 α ) r 0 / ( R α ) . and 11 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$r_{0} {/(}R\alpha {)} \ge {(4}\alpha {)}^{ - 1} .$$\end{document} r 0 / ( R α ) ≥ ( 4 α ) - 1 . The corrected balance of angular velocities requires Fig. 5 to be updated. We have plotted black dotted vertical lines for the corrected value of the equality condition from Eq. (11) and show the incorrect line from the original manuscript in red. Fig. 5 a Mean cluster radius \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\langle \vert {\mathbf {r}}-{\mathbf {\overline{r}}}\vert \rangle _{\mathrm {cl}}$$\end{document} ⟨ | r - r ¯ | ⟩ cl in units of R plotted versus torque value \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$r_0/R\alpha $$\end{document} r 0 / R α for different squirmer numbers N. b Normalized standard deviation \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varDelta N_{\mathrm {cl}}/\langle N_{\mathrm {cl}} \rangle $$\end{document} Δ N cl / ⟨ N cl ⟩ and inset: mean number of squirmers in a cluster \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\langle N_{\mathrm {cl}} \rangle $$\end{document} ⟨ N cl ⟩ . The dotted vertical lines show the equality condition of Eq. (11) for \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha =0.8$$\end{document} α = 0.8 . The red dotted line shows the erroneous condition Conclusion The angular velocity balance between Stokeslet vorticity and bottom-heaviness results in a lower bound for the rescaled torque \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$r_{0} {/(}R\alpha {)}$$\end{document} r 0 / ( R α ) that is lower than originally presented by a factor of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\frac{3}{4}$$\end{document} 3 4 . The conclusions of the original paper are unaffected.

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          Author and article information

          Contributors
          ruehle@tu-berlin.de
          Journal
          Eur Phys J E Soft Matter
          Eur Phys J E Soft Matter
          The European Physical Journal. E, Soft Matter
          Springer Berlin Heidelberg (Berlin/Heidelberg )
          1292-8941
          1292-895X
          8 July 2022
          8 July 2022
          2022
          : 45
          : 7
          : 58
          Affiliations
          GRID grid.6734.6, ISNI 0000 0001 2292 8254, Institut für Theoretische Physik, , Technische Universität Berlin, ; Hardenbergstr. 36, 10623 Berlin, Germany
          Author information
          http://orcid.org/0000-0001-6493-7204
          http://orcid.org/0000-0002-6537-3292
          http://orcid.org/0000-0002-6388-5390
          Article
          210
          10.1140/epje/s10189-022-00210-5
          9270279
          35802203
          f2e93f43-a652-4395-aba5-602a127b74d8
          © The Author(s) 2022

          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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          © EDP Sciences, SIF and Springer-Verlag GmbH Germany, part of Springer Nature 2022

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