[{"user_id":"31496","_id":"53331","language":[{"iso":"eng"}],"keyword":["General Mathematics"],"publication":"Proceedings of the Royal Society of Edinburgh: Section A Mathematics","type":"journal_article","status":"public","abstract":[{"text":"<jats:p>In a ball <jats:inline-formula><jats:alternatives><jats:tex-math>$\\Omega \\subset \\mathbb {R}^{n}$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline1.png\" /></jats:alternatives></jats:inline-formula> with <jats:inline-formula><jats:alternatives><jats:tex-math>$n\\ge 2$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline2.png\" /></jats:alternatives></jats:inline-formula>, the chemotaxis system\r\n<jats:disp-formula><jats:alternatives><jats:tex-math>\\[ \\left\\{ \\begin{array}{@{}l} u_t = \\nabla \\cdot \\big( D(u)\\nabla u\\big) + \\nabla\\cdot \\big(\\dfrac{u}{v} \\nabla v\\big), \\\\ 0=\\Delta v - uv \\end{array} \\right. \\]</jats:tex-math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" position=\"float\" xlink:href=\"S0308210522000397_eqnU1.png\" /></jats:alternatives></jats:disp-formula>is considered along with no-flux boundary conditions for <jats:inline-formula><jats:alternatives><jats:tex-math>$u$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline3.png\" /></jats:alternatives></jats:inline-formula> and with prescribed constant positive Dirichlet boundary data for <jats:inline-formula><jats:alternatives><jats:tex-math>$v$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline4.png\" /></jats:alternatives></jats:inline-formula>. It is shown that if <jats:inline-formula><jats:alternatives><jats:tex-math>$D\\in C^{3}([0,\\infty ))$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline5.png\" /></jats:alternatives></jats:inline-formula> is such that <jats:inline-formula><jats:alternatives><jats:tex-math>$0&lt; D(\\xi ) \\le {K_D} (\\xi +1)^{-\\alpha }$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline6.png\" /></jats:alternatives></jats:inline-formula> for all <jats:inline-formula><jats:alternatives><jats:tex-math>$\\xi &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline7.png\" /></jats:alternatives></jats:inline-formula> with some <jats:inline-formula><jats:alternatives><jats:tex-math>${K_D}&gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline8.png\" /></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$\\alpha &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline9.png\" /></jats:alternatives></jats:inline-formula>, then for all initial data from a considerably large set of radial functions on <jats:inline-formula><jats:alternatives><jats:tex-math>$\\Omega$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline10.png\" /></jats:alternatives></jats:inline-formula>, the corresponding initial-boundary value problem admits a solution blowing up in finite time.</jats:p>","lang":"eng"}],"volume":153,"date_created":"2024-04-07T12:44:26Z","author":[{"last_name":"Wang","full_name":"Wang, Yulan","first_name":"Yulan"},{"first_name":"Michael","full_name":"Winkler, Michael","last_name":"Winkler"}],"date_updated":"2024-04-07T12:44:30Z","publisher":"Cambridge University Press (CUP)","doi":"10.1017/prm.2022.39","title":"Finite-time blow-up in a repulsive chemotaxis-consumption system","issue":"4","publication_identifier":{"issn":["0308-2105","1473-7124"]},"publication_status":"published","page":"1150-1166","intvolume":"       153","citation":{"mla":"Wang, Yulan, and Michael Winkler. “Finite-Time Blow-up in a Repulsive Chemotaxis-Consumption System.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 153, no. 4, Cambridge University Press (CUP), 2022, pp. 1150–66, doi:<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>.","short":"Y. Wang, M. Winkler, Proceedings of the Royal Society of Edinburgh: Section A Mathematics 153 (2022) 1150–1166.","bibtex":"@article{Wang_Winkler_2022, title={Finite-time blow-up in a repulsive chemotaxis-consumption system}, volume={153}, DOI={<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>}, number={4}, journal={Proceedings of the Royal Society of Edinburgh: Section A Mathematics}, publisher={Cambridge University Press (CUP)}, author={Wang, Yulan and Winkler, Michael}, year={2022}, pages={1150–1166} }","apa":"Wang, Y., &#38; Winkler, M. (2022). Finite-time blow-up in a repulsive chemotaxis-consumption system. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, <i>153</i>(4), 1150–1166. <a href=\"https://doi.org/10.1017/prm.2022.39\">https://doi.org/10.1017/prm.2022.39</a>","ama":"Wang Y, Winkler M. Finite-time blow-up in a repulsive chemotaxis-consumption system. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>. 2022;153(4):1150-1166. doi:<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>","chicago":"Wang, Yulan, and Michael Winkler. “Finite-Time Blow-up in a Repulsive Chemotaxis-Consumption System.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i> 153, no. 4 (2022): 1150–66. <a href=\"https://doi.org/10.1017/prm.2022.39\">https://doi.org/10.1017/prm.2022.39</a>.","ieee":"Y. Wang and M. Winkler, “Finite-time blow-up in a repulsive chemotaxis-consumption system,” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 153, no. 4, pp. 1150–1166, 2022, doi: <a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>."},"year":"2022"},{"language":[{"iso":"eng"}],"_id":"63274","user_id":"31496","abstract":[{"text":"<jats:p>In a ball <jats:inline-formula><jats:alternatives><jats:tex-math>$\\Omega \\subset \\mathbb {R}^{n}$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline1.png\" /></jats:alternatives></jats:inline-formula> with <jats:inline-formula><jats:alternatives><jats:tex-math>$n\\ge 2$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline2.png\" /></jats:alternatives></jats:inline-formula>, the chemotaxis system\r\n<jats:disp-formula><jats:alternatives><jats:tex-math>\\[ \\left\\{ \\begin{array}{@{}l} u_t = \\nabla \\cdot \\big( D(u)\\nabla u\\big) + \\nabla\\cdot \\big(\\dfrac{u}{v} \\nabla v\\big), \\\\ 0=\\Delta v - uv \\end{array} \\right. \\]</jats:tex-math><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" position=\"float\" xlink:href=\"S0308210522000397_eqnU1.png\" /></jats:alternatives></jats:disp-formula>is considered along with no-flux boundary conditions for <jats:inline-formula><jats:alternatives><jats:tex-math>$u$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline3.png\" /></jats:alternatives></jats:inline-formula> and with prescribed constant positive Dirichlet boundary data for <jats:inline-formula><jats:alternatives><jats:tex-math>$v$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline4.png\" /></jats:alternatives></jats:inline-formula>. It is shown that if <jats:inline-formula><jats:alternatives><jats:tex-math>$D\\in C^{3}([0,\\infty ))$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline5.png\" /></jats:alternatives></jats:inline-formula> is such that <jats:inline-formula><jats:alternatives><jats:tex-math>$0&lt; D(\\xi ) \\le {K_D} (\\xi +1)^{-\\alpha }$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline6.png\" /></jats:alternatives></jats:inline-formula> for all <jats:inline-formula><jats:alternatives><jats:tex-math>$\\xi &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline7.png\" /></jats:alternatives></jats:inline-formula> with some <jats:inline-formula><jats:alternatives><jats:tex-math>${K_D}&gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline8.png\" /></jats:alternatives></jats:inline-formula> and <jats:inline-formula><jats:alternatives><jats:tex-math>$\\alpha &gt;0$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline9.png\" /></jats:alternatives></jats:inline-formula>, then for all initial data from a considerably large set of radial functions on <jats:inline-formula><jats:alternatives><jats:tex-math>$\\Omega$</jats:tex-math><jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0308210522000397_inline10.png\" /></jats:alternatives></jats:inline-formula>, the corresponding initial-boundary value problem admits a solution blowing up in finite time.</jats:p>","lang":"eng"}],"status":"public","type":"journal_article","publication":"Proceedings of the Royal Society of Edinburgh: Section A Mathematics","title":"Finite-time blow-up in a repulsive chemotaxis-consumption system","doi":"10.1017/prm.2022.39","date_updated":"2025-12-18T20:11:15Z","publisher":"Cambridge University Press (CUP)","author":[{"last_name":"Wang","full_name":"Wang, Yulan","first_name":"Yulan"},{"first_name":"Michael","id":"31496","full_name":"Winkler, Michael","last_name":"Winkler"}],"date_created":"2025-12-18T19:14:20Z","volume":153,"year":"2022","citation":{"ieee":"Y. Wang and M. Winkler, “Finite-time blow-up in a repulsive chemotaxis-consumption system,” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 153, no. 4, pp. 1150–1166, 2022, doi: <a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>.","chicago":"Wang, Yulan, and Michael Winkler. “Finite-Time Blow-up in a Repulsive Chemotaxis-Consumption System.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i> 153, no. 4 (2022): 1150–66. <a href=\"https://doi.org/10.1017/prm.2022.39\">https://doi.org/10.1017/prm.2022.39</a>.","ama":"Wang Y, Winkler M. Finite-time blow-up in a repulsive chemotaxis-consumption system. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>. 2022;153(4):1150-1166. doi:<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>","bibtex":"@article{Wang_Winkler_2022, title={Finite-time blow-up in a repulsive chemotaxis-consumption system}, volume={153}, DOI={<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>}, number={4}, journal={Proceedings of the Royal Society of Edinburgh: Section A Mathematics}, publisher={Cambridge University Press (CUP)}, author={Wang, Yulan and Winkler, Michael}, year={2022}, pages={1150–1166} }","mla":"Wang, Yulan, and Michael Winkler. “Finite-Time Blow-up in a Repulsive Chemotaxis-Consumption System.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 153, no. 4, Cambridge University Press (CUP), 2022, pp. 1150–66, doi:<a href=\"https://doi.org/10.1017/prm.2022.39\">10.1017/prm.2022.39</a>.","short":"Y. Wang, M. Winkler, Proceedings of the Royal Society of Edinburgh: Section A Mathematics 153 (2022) 1150–1166.","apa":"Wang, Y., &#38; Winkler, M. (2022). Finite-time blow-up in a repulsive chemotaxis-consumption system. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, <i>153</i>(4), 1150–1166. <a href=\"https://doi.org/10.1017/prm.2022.39\">https://doi.org/10.1017/prm.2022.39</a>"},"page":"1150-1166","intvolume":"       153","publication_status":"published","publication_identifier":{"issn":["0308-2105","1473-7124"]},"issue":"4"},{"type":"journal_article","publication":"Proceedings of the Royal Society of Edinburgh: Section A Mathematics","status":"public","abstract":[{"text":"<jats:p>The paper studies large time behaviour of solutions to the Keller–Segel system with quadratic degradation in a liquid environment, as given by</jats:p><jats:p><jats:disp-formula><jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" orientation=\"portrait\" mime-subtype=\"gif\" mimetype=\"image\" position=\"float\" xlink:type=\"simple\" xlink:href=\"S0308210518000057_equ01\" /></jats:disp-formula></jats:p><jats:p>under Neumann boundary conditions in a bounded domain <jats:italic>Ω ⊂</jats:italic> ℝ<jats:sup><jats:italic>n</jats:italic></jats:sup>, where <jats:italic>n</jats:italic> ≥ 1 is arbitrary. It is shown that whenever <jats:italic>U</jats:italic> : <jats:italic>Ω ×</jats:italic> (0,<jats:italic>∞</jats:italic>) <jats:italic>→</jats:italic> ℝ<jats:sup><jats:italic>n</jats:italic></jats:sup> is a bounded and sufficiently regular solenoidal vector field any non-trivial global bounded solution of (<jats:italic>⋆</jats:italic>) approaches the trivial equilibrium at a rate that, with respect to the norm in either of the spaces <jats:italic>L</jats:italic><jats:sup>1</jats:sup>(<jats:italic>Ω</jats:italic>) and <jats:italic>L<jats:sup>∞</jats:sup></jats:italic>(<jats:italic>Ω</jats:italic>), can be controlled from above and below by appropriate multiples of 1<jats:italic>/</jats:italic>(<jats:italic>t</jats:italic> + 1). This underlines that, even up to this quantitative level of accuracy, the large time behaviour in (<jats:italic>⋆</jats:italic>) is essentially independent not only of the particular fluid flow, but also of any effect originating from chemotactic cross-diffusion. The latter is in contrast to the corresponding Cauchy problem, for which known results show that in the <jats:italic>n</jats:italic> = 2 case the presence of chemotaxis can significantly enhance biomixing by reducing the respective spatial <jats:italic>L</jats:italic><jats:sup>1</jats:sup> norms of solutions.</jats:p>","lang":"eng"}],"user_id":"31496","_id":"63369","language":[{"iso":"eng"}],"issue":"5","publication_status":"published","publication_identifier":{"issn":["0308-2105","1473-7124"]},"citation":{"apa":"Cao, X., &#38; Winkler, M. (2018). Sharp decay estimates in a bioconvection model with quadratic degradation in bounded domains. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, <i>148</i>(5), 939–955. <a href=\"https://doi.org/10.1017/s0308210518000057\">https://doi.org/10.1017/s0308210518000057</a>","short":"X. Cao, M. Winkler, Proceedings of the Royal Society of Edinburgh: Section A Mathematics 148 (2018) 939–955.","mla":"Cao, Xinru, and Michael Winkler. “Sharp Decay Estimates in a Bioconvection Model with Quadratic Degradation in Bounded Domains.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 148, no. 5, Cambridge University Press (CUP), 2018, pp. 939–55, doi:<a href=\"https://doi.org/10.1017/s0308210518000057\">10.1017/s0308210518000057</a>.","bibtex":"@article{Cao_Winkler_2018, title={Sharp decay estimates in a bioconvection model with quadratic degradation in bounded domains}, volume={148}, DOI={<a href=\"https://doi.org/10.1017/s0308210518000057\">10.1017/s0308210518000057</a>}, number={5}, journal={Proceedings of the Royal Society of Edinburgh: Section A Mathematics}, publisher={Cambridge University Press (CUP)}, author={Cao, Xinru and Winkler, Michael}, year={2018}, pages={939–955} }","ieee":"X. Cao and M. Winkler, “Sharp decay estimates in a bioconvection model with quadratic degradation in bounded domains,” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>, vol. 148, no. 5, pp. 939–955, 2018, doi: <a href=\"https://doi.org/10.1017/s0308210518000057\">10.1017/s0308210518000057</a>.","chicago":"Cao, Xinru, and Michael Winkler. “Sharp Decay Estimates in a Bioconvection Model with Quadratic Degradation in Bounded Domains.” <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i> 148, no. 5 (2018): 939–55. <a href=\"https://doi.org/10.1017/s0308210518000057\">https://doi.org/10.1017/s0308210518000057</a>.","ama":"Cao X, Winkler M. Sharp decay estimates in a bioconvection model with quadratic degradation in bounded domains. <i>Proceedings of the Royal Society of Edinburgh: Section A Mathematics</i>. 2018;148(5):939-955. doi:<a href=\"https://doi.org/10.1017/s0308210518000057\">10.1017/s0308210518000057</a>"},"intvolume":"       148","page":"939-955","year":"2018","author":[{"first_name":"Xinru","full_name":"Cao, Xinru","last_name":"Cao"},{"last_name":"Winkler","full_name":"Winkler, Michael","id":"31496","first_name":"Michael"}],"date_created":"2025-12-19T11:02:55Z","volume":148,"date_updated":"2025-12-19T11:03:03Z","publisher":"Cambridge University Press (CUP)","doi":"10.1017/s0308210518000057","title":"Sharp decay estimates in a bioconvection model with quadratic degradation in bounded domains"}]
