Finite-time blow-up in a quasilinear chemotaxis system with an external signal consumption

2019 ◽  
pp. 1
Author(s):  
Pan Zheng ◽  
Chunlai Mu ◽  
Xuegang Hu ◽  
Liangchen Wang
Keyword(s):  
Finite Time ◽  
Blow Up ◽  
External Signal ◽  
Chemotaxis System

scholarly journals Finite-Time Blow-up in a Quasilinear Degenerate Chemotaxis System with Flux Limitation

2019 ◽  
Vol 167 (1) ◽  
pp. 231-259 ◽  
Author(s):  
Yuka Chiyoda ◽  
Masaaki Mizukami ◽  
Tomomi Yokota
Keyword(s):  
Finite Time ◽  
Blow Up ◽  
Chemotaxis System ◽  
Flux Limitation

scholarly journals Global Existence and Blow-up of Classical Solution for an Attraction-repulsion Chemotaxis System with Logistic Source

2019 ◽  
pp. 1-16
Author(s):  
Lijun Yan ◽  
Zuodong Yang
Keyword(s):  
Global Existence ◽  
Boundary Conditions ◽  
Classical Solution ◽  
Finite Time ◽  
Blow Up ◽  
Smooth Boundary ◽  
Neumann Boundary ◽  
Elliptic Type ◽  
Logistic Source ◽  
Chemotaxis System

We consider the following quasilinear attraction-repulsion chemotaxis system of parabolic-elliptic-elliptic type with logistic source under homegeneous Neumann boundary conditions in a bounded domain `\Omega\subset R^{n}(n\geq2)` with smooth boundary, where`D(u)\geq c_{D}(u+1)^{m-1}` with `m\geq1`and `c_{D}>0`, `f(u)\leq a-bu^{\eta}` with `\eta>1`.{ We show two cases that the system admits a uniqueglobal bounded classical solution depending on `0\leq S(u)\leq C_{s}(u+1)^{q}, 0\leq F(u)\leq C_{F}(u+1)^{g}` by Gagliardo-Nirenberg inequality.For specific `D(u),S(u),F(u)` with logistic source for `\eta>1` and `n=2`, we establish the finite time blow-up conditions forsolutions that the finite time blow-up occurs at `x_{0}\in\Omega` whenever `\int_{\Omega}u_{0}(x)dx>\frac{8\pi}{\chi\alpha-\xi\gamma}`with `\chi\alpha-\xi\gamma>0`, under `\int_{\Omega}u_{0}(x)|x-x_{0}|^{2}dx` sufficiently small.

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