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Blow-up conditions of nonlinear parabolic equations and systems under mixed nonlinear boundary conditions
In this paper, we firstly discuss blow-up phenomena for nonlinear parabolic equations u t = ∇ ⋅ [ ρ ( u ) ∇ u ] + f ( x , t , u ) , in Ω × ( 0 , t ∗ ) , under mixed nonlinear boundary conditions ∂ u ∂ n + θ ( z ) u = h ( z , t , u ) on Γ 1 × ( 0 , t ∗ ) and u = 0 on Γ 2 × ( 0 , t ∗ ) , where Ω is a...
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Published in: | Boundary value problems 2022-06, Vol.2022 (1), p.1-19, Article 46 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | In this paper, we firstly discuss blow-up phenomena for nonlinear parabolic equations
u
t
=
∇
⋅
[
ρ
(
u
)
∇
u
]
+
f
(
x
,
t
,
u
)
,
in
Ω
×
(
0
,
t
∗
)
,
under mixed nonlinear boundary conditions
∂
u
∂
n
+
θ
(
z
)
u
=
h
(
z
,
t
,
u
)
on
Γ
1
×
(
0
,
t
∗
)
and
u
=
0
on
Γ
2
×
(
0
,
t
∗
)
, where Ω is a bounded domain and
Γ
1
and
Γ
2
are disjoint subsets of a boundary
∂
Ω. Here,
f
and
h
are real-valued
C
1
-functions and
ρ
is a positive
C
1
-function. To obtain the blow-up solutions, we introduce the following blow-up conditions:
(
C
ρ
)
:
(
2
+
ϵ
)
∫
0
u
ρ
(
w
)
f
(
x
,
t
,
w
)
d
w
≤
u
ρ
(
u
)
f
(
x
,
t
,
u
)
+
β
1
u
2
+
γ
1
,
(
2
+
ϵ
)
∫
0
u
ρ
2
(
w
)
h
(
z
,
t
,
w
)
d
w
≤
u
ρ
2
(
u
)
h
(
z
,
t
,
u
)
+
β
2
u
2
+
γ
2
,
for
x
∈
Ω
,
z
∈
∂
Ω
,
t
>
0
, and
u
∈
R
for some constants
ϵ
,
β
1
,
β
2
,
γ
1
, and
γ
2
satisfying
ϵ
>
0
,
β
1
+
λ
R
+
1
λ
S
β
2
≤
ρ
m
2
λ
R
2
ϵ
and
0
≤
β
2
≤
ρ
m
2
λ
S
2
ϵ
,
where
ρ
m
:
=
inf
s
>
0
ρ
(
s
)
,
λ
R
is the first Robin eigenvalue and
λ
S
is the first Steklov eigenvalue. Lastly, we discuss blow-up solutions for nonlinear parabolic systems. |
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ISSN: | 1687-2770 1687-2762 1687-2770 |
DOI: | 10.1186/s13661-022-01627-9 |