Finite-time blow-up in a two-dimensional Keller–Segel system with an environmental dependent logistic source

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

  • Mario Fuest

Externe Organisationen

  • Universität Paderborn
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Details

OriginalspracheEnglisch
Aufsatznummer103022
FachzeitschriftNonlinear Analysis: Real World Applications
Jahrgang52
PublikationsstatusVeröffentlicht - Apr. 2020
Extern publiziertJa

Abstract

The Neumann initial–boundary problem for the chemotaxis system u t=Δu−∇⋅(u∇v)+κ(|x|)u−μ(|x|)u p,0=Δv− [Formula presented] +u,m(t)≔∫ Ωu(⋅,t)is studied in a ball Ω=B R(0)⊂R 2, R>0 for p≥1 and sufficiently smooth functions κ,μ:[0,R]→[0,∞). We prove that whenever μ ,−κ ≥0 as well as μ(s)≤μ 1s 2p−2 for all s∈[0,R] and some μ 1>0 then for all m 0>8π there exists u 0∈C 0(Ω¯) with ∫ Ωu 0=m 0 and a solution (u,v) to (⋆) with initial datum u 0 blowing up in finite time. If in addition κ≡0 then all solutions with initial mass smaller than 8π are global in time, displaying a certain critical mass phenomenon. On the other hand, if p>2, we show that for all μ satisfying μ(s)≥μ 1s p−2−ε for all s∈[0,R] and some μ 1,ε>0 the system (⋆) admits a global classical solution for each initial datum 0≤u 0∈C 0(Ω¯).

Zitieren

Finite-time blow-up in a two-dimensional Keller–Segel system with an environmental dependent logistic source. / Fuest, Mario.
in: Nonlinear Analysis: Real World Applications, Jahrgang 52, 103022, 04.2020.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Download
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title = "Finite-time blow-up in a two-dimensional Keller–Segel system with an environmental dependent logistic source",
abstract = "The Neumann initial–boundary problem for the chemotaxis system u t=Δu−∇⋅(u∇v)+κ(|x|)u−μ(|x|)u p,0=Δv− [Formula presented] +u,m(t)≔∫ Ωu(⋅,t)is studied in a ball Ω=B R(0)⊂R 2, R>0 for p≥1 and sufficiently smooth functions κ,μ:[0,R]→[0,∞). We prove that whenever μ ′,−κ ′≥0 as well as μ(s)≤μ 1s 2p−2 for all s∈[0,R] and some μ 1>0 then for all m 0>8π there exists u 0∈C 0(Ω¯) with ∫ Ωu 0=m 0 and a solution (u,v) to (⋆) with initial datum u 0 blowing up in finite time. If in addition κ≡0 then all solutions with initial mass smaller than 8π are global in time, displaying a certain critical mass phenomenon. On the other hand, if p>2, we show that for all μ satisfying μ(s)≥μ 1s p−2−ε for all s∈[0,R] and some μ 1,ε>0 the system (⋆) admits a global classical solution for each initial datum 0≤u 0∈C 0(Ω¯).",
keywords = "Chemotaxis, Critical mass, Finite-time blow-up, Logistic source",
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T1 - Finite-time blow-up in a two-dimensional Keller–Segel system with an environmental dependent logistic source

AU - Fuest, Mario

N1 - Publisher Copyright: © 2019 Elsevier Ltd

PY - 2020/4

Y1 - 2020/4

N2 - The Neumann initial–boundary problem for the chemotaxis system u t=Δu−∇⋅(u∇v)+κ(|x|)u−μ(|x|)u p,0=Δv− [Formula presented] +u,m(t)≔∫ Ωu(⋅,t)is studied in a ball Ω=B R(0)⊂R 2, R>0 for p≥1 and sufficiently smooth functions κ,μ:[0,R]→[0,∞). We prove that whenever μ ′,−κ ′≥0 as well as μ(s)≤μ 1s 2p−2 for all s∈[0,R] and some μ 1>0 then for all m 0>8π there exists u 0∈C 0(Ω¯) with ∫ Ωu 0=m 0 and a solution (u,v) to (⋆) with initial datum u 0 blowing up in finite time. If in addition κ≡0 then all solutions with initial mass smaller than 8π are global in time, displaying a certain critical mass phenomenon. On the other hand, if p>2, we show that for all μ satisfying μ(s)≥μ 1s p−2−ε for all s∈[0,R] and some μ 1,ε>0 the system (⋆) admits a global classical solution for each initial datum 0≤u 0∈C 0(Ω¯).

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KW - Chemotaxis

KW - Critical mass

KW - Finite-time blow-up

KW - Logistic source

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