A hyperbolic–elliptic–elliptic system of an attraction–repulsion chemotaxis model with nonlinear productions
This paper studies the hyperbolic–elliptic–elliptic system of an attraction–repulsion chemotaxis model with nonlinear productions and logistic source: u t = - χ ∇ · ( u ∇ v ) + ξ ∇ · ( u ∇ w ) + μ u ( 1 - u k ) , 0 = Δ v + α u q - β v , 0 = Δ w + γ u r - δ w , in a bounded domain Ω ⊂ R n , n ≥ 1 , s...
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Veröffentlicht in: | Journal of evolution equations 2018-06, Vol.18 (2), p.973-1001 |
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Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
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Zusammenfassung: | This paper studies the hyperbolic–elliptic–elliptic system of an attraction–repulsion chemotaxis model with nonlinear productions and logistic source:
u
t
=
-
χ
∇
·
(
u
∇
v
)
+
ξ
∇
·
(
u
∇
w
)
+
μ
u
(
1
-
u
k
)
,
0
=
Δ
v
+
α
u
q
-
β
v
,
0
=
Δ
w
+
γ
u
r
-
δ
w
, in a bounded domain
Ω
⊂
R
n
,
n
≥
1
, subject to the non-flux boundary condition. We at first establish the local existence of solutions (the so-called strong
W
1
,
p
-solutions, satisfying the hyperbolic equation weakly and solving the elliptic ones classically) to the model via applying the viscosity vanishing method and then give criteria on global boundedness versus finite- time blowup for them. It is proved that if the attraction is dominated by the logistic source or the repulsion with
max
{
r
,
k
}
>
q
, the solutions would be globally bounded; otherwise, the finite-time blowup of solutions may occur whenever
max
{
r
,
k
}
<
q
. Under the balance situations with
q
=
r
=
k
,
q
=
r
>
k
or
q
=
k
>
r
, the boundedness or possible finite-time blowup would depend on the sizes of the coefficients involved. |
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ISSN: | 1424-3199 1424-3202 |
DOI: | 10.1007/s00028-018-0428-4 |