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Chemotaxis systems with singular sensitivity and logistic source: Boundedness, persistence, absorbing set, and entire solutions
Authors
Halil Ibrahim Kurt
Wenxian Shen
Publication date
3 March 2024
Publisher
View
on
arXiv
Abstract
This paper deals with the following parabolic-elliptic chemotaxis system with singular sensitivity and logistic source, \begin{equation} \begin{cases} u_t=\Delta u-\chi\nabla\cdot (\frac{u}{v} \nabla v)+u(a(t,x)-b(t,x) u), & x\in \Omega,\cr 0=\Delta v- \mu v+ \nu u, & x\in \Omega, \cr \frac{\partial u}{\partial n}=\frac{\partial v}{\partial n}=0, & x\in\partial\Omega, \end{cases} \end{equation} where
Ξ©
β
R
N
\Omega \subset \mathbb{R}^N
Ξ©
β
R
N
is a smooth bounded domain,
a
(
t
,
x
)
a(t,x)
a
(
t
,
x
)
and
b
(
t
,
x
)
b(t,x)
b
(
t
,
x
)
are positive smooth functions, and
Ο
\chi
Ο
,
ΞΌ
\mu
ΞΌ
and
Ξ½
\nu
Ξ½
are positive constants. In the very recent paper [25], we proved that for given nonnegative initial function
0
β‘ΜΈ
u
0
β
C
0
(
Ξ©
Λ
)
0\not\equiv u_0\in C^0(\bar \Omega)
0
ξ
β‘
u
0
β
β
C
0
(
Ξ©
Λ
)
and
s
β
R
s\in\mathbb{R}
s
β
R
, (0.1) has a unique globally defined classical solution
(
u
(
t
,
x
;
s
,
u
0
)
,
v
(
t
,
x
;
s
,
u
0
)
)
(u(t,x;s,u_0),v(t,x;s,u_0))
(
u
(
t
,
x
;
s
,
u
0
β
)
,
v
(
t
,
x
;
s
,
u
0
β
))
with
u
(
s
,
x
;
s
,
u
0
)
=
u
0
(
x
)
u(s,x;s,u_0)=u_0(x)
u
(
s
,
x
;
s
,
u
0
β
)
=
u
0
β
(
x
)
, provided that
a
inf
β‘
=
inf
β‘
t
β
R
,
x
β
Ξ©
a
(
t
,
x
)
a_{\inf}=\inf_{t\in\mathbb{R},x\in\Omega}a(t,x)
a
i
n
f
β
=
in
f
t
β
R
,
x
β
Ξ©
β
a
(
t
,
x
)
is large relative to
Ο
\chi
Ο
and
u
0
u_0
u
0
β
is not small. In this paper, we further investigate qualitative properties of globally defined positive solutions of (0.1) under the assumption that
a
inf
β‘
a_{\inf}
a
i
n
f
β
is large relative to
Ο
\chi
Ο
and
u
0
u_0
u
0
β
is not small. Among others, we provide some concrete estimates for
β«
Ξ©
u
β
p
\int_\Omega u^{-p}
β«
Ξ©
β
u
β
p
and
β«
Ξ©
u
q
\int_\Omega u^q
β«
Ξ©
β
u
q
for some
p
>
0
p>0
p
>
0
and
q
>
max
β‘
{
2
,
N
}
q>\max\{2,N\}
q
>
max
{
2
,
N
}
and prove that any globally defined positive solution is bounded above and below eventually by some positive constants independent of its initial functions. We prove the existence of a ``rectangular'' type bounded invariant set (in
L
q
L^q
L
q
) which eventually attracts all the globally defined positive solutions. We also prove that (0.1) has a positive entire classical solution
(
u
β
(
t
,
x
)
,
v
β
(
t
,
x
)
)
(u^*(t,x),v^*(t,x))
(
u
β
(
t
,
x
)
,
v
β
(
t
,
x
))
, which is periodic in
t
t
t
if
a
(
t
,
x
)
a(t,x)
a
(
t
,
x
)
and
b
(
t
,
x
)
b(t,x)
b
(
t
,
x
)
are periodic in
t
t
t
and is independent of
t
t
t
if
a
(
t
,
x
)
a(t,x)
a
(
t
,
x
)
and
b
(
t
,
x
)
b(t,x)
b
(
t
,
x
)
are independent of
t
t
t
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oai:arXiv.org:2205.00096
Last time updated on 22/07/2022