Access the full text.
Sign up today, get DeepDyve free for 14 days.
N. Bellomo, M. Winkler (2017)
Finite-time blow-up in a degenerate chemotaxis system with flux limitation, 4
Dirk Horstmann, M. Winkler (2005)
Boundedness vs. blow-up in a chemotaxis systemJournal of Differential Equations, 215
E. Keller, L. Segel (1971)
Traveling bands of chemotactic bacteria: a theoretical analysis.Journal of theoretical biology, 30 2
T. Hashira, Sachiko Ishida, T. Yokota (2018)
Finite-time blow-up for quasilinear degenerate Keller-Segel systems of parabolic-parabolic typeJournal of Differential Equations, 264
Tomasz Cieślak, Christian Stinner (2012)
Finite-Time Blowup in a Supercritical Quasilinear Parabolic-Parabolic Keller-Segel System in Dimension 2Acta Applicandae Mathematicae, 129
Tomasz Cie'slak, Christian Stinner (2014)
New critical exponents in a fully parabolic quasilinear Keller–Segel system and applications to volume filling modelsJournal of Differential Equations, 258
N. Bellomo, M. Winkler (2016)
A degenerate chemotaxis system with flux limitation: Maximally extended solutions and absence of gradient blow-upCommunications in Partial Differential Equations, 42
(2001)
Finite dimensional attractor for one-dimensional Keller–Segel equations
J. Lankeit (2017)
Infinite time blow-up of many solutions to a general quasilinear parabolic-elliptic Keller-Segel systemDiscrete & Continuous Dynamical Systems - S
M. Winkler (2011)
Finite-time blow-up in the higher-dimensional parabolic-parabolic Keller-Segel systemarXiv: Analysis of PDEs
T. Hillen, K Painter, K. Painter
A User's Guide to Pde Models for Chemotaxis
三村 与士文 (2012)
The variational formulation of the fully parabolic Keller-Segel system with degenerate diffusion
Youshan Tao, M. Winkler (2011)
Boundedness in a quasilinear parabolic-parabolic Keller-Segel system with subcritical sensitivityJournal of Differential Equations, 252
Tomasz Cieślak, M. Winkler (2008)
Finite-time blow-up in a quasilinear system of chemotaxisNonlinearity, 21
Sachiko Ishida, T. Yokota (2012)
Global existence of weak solutions to quasilinear degenerate Keller-Segel systems of parabolic-parabolic type with small dataJournal of Differential Equations, 252
Dirk Horstmann, Guofang Wang (2001)
Blow-up in a chemotaxis model without symmetry assumptionsEuropean Journal of Applied Mathematics, 12
M. Winkler, Kianhwa Djie (2010)
Boundedness and finite-time collapse in a chemotaxis system with volume-filling effectNonlinear Analysis-theory Methods & Applications, 72
P. Laurençot, N. Mizoguchi (2017)
Finite time blowup for the parabolic–parabolic Keller–Segel system with critical diffusionAnnales De L Institut Henri Poincare-analyse Non Lineaire, 34
(1997)
Application of the Trudinger–Moser inequality to a parabolic system of chemotaxis
Sachiko Ishida, Kiyotaka Seki, T. Yokota (2014)
Boundedness in quasilinear Keller–Segel systems of parabolic–parabolic type on non-convex bounded domainsJournal of Differential Equations, 256
Tomasz Cie'slak, Christian Stinner (2011)
Finite-time blowup and global-in-time unbounded solutions to a parabolic–parabolic quasilinear Keller–Segel system in higher dimensionsJournal of Differential Equations, 252
Xinru Cao (2014)
Global bounded solutions of the higher-dimensional Keller-Segel system under smallness conditions in optimal spacesarXiv: Analysis of PDEs
M. Mizukami, Tatsuhiko Ono, T. Yokota (2019)
Extensibility criterion ruling out gradient blow-up in a quasilinear degenerate chemotaxis system with flux limitationJournal of Differential Equations
This paper deals with the quasilinear degenerate chemotaxis system with flux limitation{ut=∇⋅(up∇uu2+|∇u|2)−χ∇⋅(uq∇v1+|∇v|2),x∈Ω,t>0,0=Δv−μ+u,x∈Ω,t>0,\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document} $$\begin{aligned} \textstyle\begin{cases} u_{t} = \nabla \cdot \biggl(\frac{u^{p} \nabla u}{\sqrt{u^{2} + | \nabla u|^{2}}} \biggr) -\chi \nabla \cdot \biggl( \frac{u^{q} \nabla v}{\sqrt{1 + |\nabla v|^{2}}} \biggr), &x\in \varOmega ,\ t>0, \\ 0 = \Delta v - \mu + u, &x\in \varOmega ,\ t>0, \end{cases}\displaystyle \end{aligned}$$ \end{document} where Ω:=BR(0)⊂Rn\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$\varOmega := B_{R}(0) \subset \mathbb{R}^{n}$\end{document} (n∈N\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$n \in \mathbb{N}$\end{document}) is a ball with some R>0\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$R>0$\end{document}, and χ>0\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$\chi >0$\end{document}, p,q≥1\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$p,q\geq 1$\end{document}, μ:=1|Ω|∫Ωu0\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$\mu := \frac{1}{| \varOmega |} \int _{\varOmega }u_{0}$\end{document} and u0\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$u_{0}$\end{document} is an initial data of an unknown function u\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$u$\end{document}. Bellomo–Winkler (Trans. Am. Math. Soc. Ser. B 4, 31–67, 2017) established existence of an initial data such that the corresponding solution blows up in finite time when p=q=1\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$p=q=1$\end{document}. This paper gives existence of blow-up solutions under some condition for χ\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$\chi $\end{document} and u0\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$u_{0}$\end{document} when 1≤p≤q\documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$1\leq p\leq q$\end{document}.
Acta Applicandae Mathematicae – Springer Journals
Published: Jun 8, 2020
Read and print from thousands of top scholarly journals.
Already have an account? Log in
Bookmark this article. You can see your Bookmarks on your DeepDyve Library.
To save an article, log in first, or sign up for a DeepDyve account if you don’t already have one.
Copy and paste the desired citation format or use the link below to download a file formatted for EndNote
Access the full text.
Sign up today, get DeepDyve free for 14 days.
All DeepDyve websites use cookies to improve your online experience. They were placed on your computer when you launched this website. You can change your cookie settings through your browser.