Báo cáo hóa học: " Research Article On a Mixed Nonlinear One Point Boundary Value Problem for an Integrodifferential Equation" - Pdf 15

Hindawi Publishing Corporation
Boundary Value Problems
Volume 2008, Article ID 814947, 8 pages
doi:10.1155/2008/814947
Research Article
On a Mixed Nonlinear One Point Boundary Value
Problem for an Integrodifferential Equation
Said Mesloub
Department of Mathematics, College of Sciences, King Saud University, P.O. Box 2455,
Riyadh 11451, Saudi Arabia
Correspondence should be addressed to Said Mesloub, [email protected]
Received 31 August 2007; Accepted 5 February 2008
Recommended by Martin Schechter
This paper is devoted to the study of a mixed problem for a nonlinear parabolic integro-differential
equation which mainly arise from a one dimensional quasistatic contact problem. We prove the
existence and uniqueness of solutions in a weighted Sobolev space. Proofs are based on some a
priori estimates and on the Schauder fixed point theorem. we also give a result which helps to
establish the regularity of a solution.
Copyright q 2008 Said Mesloub. This is an open access article distributed under the Creative
Commons Attribution License, which permits unrestricted use, distribution, and reproduction in
any medium, provided the original work is properly cited.
1. Introduction
In this paper, we are concerned with a one-dimensional nonlinear parabolic integrodifferential
equation with Bessel operator, having the form
u
t
− u
xx

1
x

2 Boundary Value Problems
equation with Bessel operator supplemented with a one point boundary condition and an
initial condition. The proof is established by exploiting some a priori estimates and using a
fixed point argument.
2. The problem
We consider the following problem:
u
t
− u
xx

1
x
u
x

d
dt
max


x
0
ξuξ, tdξ, 0

 f, x, t ∈ Q
T
0, 1 × 0,T, 2.1
u
x

 are given by
u, v
L
2
ρ
Q
T



Q
T
xuv dx dt, u, v
L
2
σ
Q
T



Q
T
x
2
uv dx dt, 2.4
Let W
1,0
σ,2
Q

T

, 2.5
and V
σ
 W
2,1
σ,2
Q
T
 be the subspace of W
1,0
σ,2
Q
T
 whose elements satisfy u
t
,u
xx
∈ L
2
σ
Q
T
.In
general, a function in the space W
i,j
σ,p
Q
T

σ

0, 1

,W
1
σ,2

0, 1

 H
1
σ

0, 1

,W
0,0
σ,2

Q
T

 L
2
σ

Q
T


T







x
0
uξ, tdξ




2
L
2
Q
T


1
2
u
2
L
2
Q
T

.
Proof. Let u
1
and u
2
be two solutions of the problem 2.1–2.3 and let θx, tw
1
x, t −
w
2
x, t,where
w
i
x, t

t
0
u
i
x, τdτ, i  1, 2, 3.1
then the function θx, t satisfies
Lθ  θ
t

1
x


x


x
0
ξu
i
ξ, tdξ, 0

,i 1, 2, 3.5
then calculating the two integrals

Q
T
2x
2
θLθdxdt,

Q
T
2x
2
θ
t
Lθdxdt,using conditions 3.3,
3.4, and a combining with −

Q
T
2xθ
x
Lθdxdt,we obtain
2

θ
x


2
L
2
Q
T




θ·,T


2
L
2
σ
0,1



θ
x
·,T


2

2

θ, β
1
− β
2

L
2
σ
Q
T

− 2

θ
x

1
− β
2

L
2
ρ
Q
T

.
3.6

2
Q
T

,
2

θ, β
1
− β
2

L
2
σ
Q
T

≤ 4θ
2
L
2
σ
Q
T


1
8



θ
t


2
L
2
σ
Q
T


1
2


θ
t


2
L
2
σ
Q
T

,
−2

8


θ
t


2
L
2
σ
Q
T

.
3.7
4 Boundary Value Problems
Therefore, using inequalities 3.7,weinferfrom3.6


θ
t


2
L
2
σ
Q
T

Q
T

 20


θ
x


2
L
2
σ
Q
T

. 3.8
By applying Gronwall’s lemma to 3.8, we conclude that


θ
t


2
L
2
σ
Q

σ,2
0,1
≤ c
2
2
, 3.10
for c
2
> 0 small enough and that
g
x
10. 3.11
Then there exists at least one solution ux, t ∈ W
2,1
σ,2
Q
T
 of problem 2.1–2.3.
Proof. We define, for positive constants C and D which will be specified later, a class of
functions W  WC, D which consists of all functions v ∈ L
2
σ
Q
T
 satisfying conditions 2.2,
2.3,and
v
V
σ
≤ C,

ux, 0gx,x∈ 0, 1,
3.13
where
Jv 
d
dt
max


x
0
ξvξ, tdξ, 0

, 3.14
has a unique solution u ∈ V
σ
. We define a mapping h such that u  hv.
Once it is proved that the mapping h has a fixed point u in the closed bounded convex
subset WC, D, then u is the desired solution.
Said Mesloub 5
We, first, show that h maps WC, D into itself. For this purpose we write u in the form
u  w  ζ, where w is a solution of the problem
w
t
− w
xx

1
x
w

2
w
t
− 6xw
x
and
O
2
ζ  2x
2
ζ  2x
2
ζ
t
− 6xζ
x
, then integrating over Q
T
, we obtain
2Lw, w
L
2
σ
Q
T

 2

Lw, w
t

L
2
σ
Q
T

− 6

Jv,w
x

L
2
ρ
Q
T
,
3.21
2Lζ, ζ
L
2
σ
Q
T

 2

Lζ, ζ
t


2
σ
Q
T

− 6

f, ζ
x

L
2
ρ
Q
T

.
3.22
By using conditions 3.16, 3.17, 3.19, 3.20, an evaluation of the left-hand side of both
equalities 3.21 and 3.22 gives, respectively,


wx, T


2
L
2
σ
0.1

x, T


2
L
2
σ
0.1
2


w
t


2
L
2
σ
Q
T

 2

w
t
,w
x

L


 2Jv,w
L
2
σ
Q
T

 2

Jv,w
t

L
2
σ
Q
T

− 6

Jv,w
x

L
2
ρ
Q
T


w
2
V
σ
≤ 7exp7T


Jv


2
L
2
σ
Q
T

.
3.25
6 Boundary Value Problems
We also multiply by x and square both sides of 3.15 , integrate over Q
T
, use the integral
−2

Q
T
xw
x
Lwdxdt,then integrate by parts and using inequality 2.7,weobtain

w
x
·,T


2
L
2
σ
Q
T

≤ 2Jv
L
2
σ
Q
T

. 3.26
Direct computations yield
Jv
2
L
2
σ
Q
T



σ
≤ 2w
2
V
σ
 2ζ
2
V
σ
≤ 14 exp7T

c
2
2
 c
2
1

,


u
t


2
L
2
σ
Q

4c
2
1
 14 exp7Tc
2
2
.
3.29
At this point we take C ≥

14 exp7T/2

c
2
1
 c
2
2
 and D ≥

4c
2
1
 14 exp7Tc
2
2
, so that it
follows from the last two inequalities that u
V
σ

1
x
U
x

d
dt
max


x
0
ξv
1
ξ, tdξ, 0


d
dt
max


x
0
ξv
2
ξ, tdξ, 0

,
U


x
0
ξv
2
ξ, tdξ, 0

,
p
x
1,t0,px, 00.
3.32
Since
F
2
L
2
σ
Q
T




v
1
− v
2



Q
T

, 3.34
Said Mesloub 7
or


hv
1
− hv
2


2
L
2
σ
Q
T

≤ 6


v
1
− v
2



0,T; E
1

3.36
is compactly embedded in L
p
0,T; E, that is, the bounded sets are relatively compact in L
p
0,T; E.
Note that L
2
σ
0,T; L
2
σ
0, 1  L
2
σ
Q
T
, hWC, D ⊂ WC, D ⊂ L
2
σ
Q
T
. By the Schauder
fixed point theorem the mapping h has a fixed point u in WC, D.
Remark 3.4. For compactness of the set
WC, D, see also 8, 9.
Remark 3.5. The following theorem gives an a priori estimate which may be used in establishing

2
L
2
σ
Q
T




u
xx


2
L
2
σ
Q
T




u
x


2
L


2
L
2
σ
Q
T




u
xx


2
L
2
σ
Q
T




u
x
·,T



Q
T
x
2

d
dt
max


x
0
ξuξ, tdξ, 0

 f

2
dx dt.
3.38
Multiplying 2.1 by 2x
2
u
t
, integrating over Q
T
, carrying out standard integrations by parts,
and using conditions 2.2 and 2.3 yields
2




L
2
ρ
Q
T




g
x


2
L
2
σ
0,1
 2

Q
T
x
2
u
t
fdxdt 2

Q

σ
Q
T




u
xx


2
L
2
σ
Q
T

 2


u
x
·,T


2
L
2
σ

2
L
2
σ
0,1

1
8


u
t


2
L
2
σ
Q
T


1
8
u
2
L
2
σ
Q

L
2
σ
0,1



u
x
·,T


2
L
2
σ
0,1



u
t


2
L
2
σ
Q
T


g
2
W
1
σ,2
0,1
 f
2
L
2
σ
Q
T

 u
2
L
2
σ
Q
T




u
x



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6 L. Garding, Cauchy Problem for Hyperbolic Equations, Lecture Notes, University of Chicago, Chicago, Ill,
USA, 1957.
7 J. Simon, “Compact sets in the space L
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0,T; B,” Annali di Matematica Pura ed Applicata, vol. 146, no. 1,
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eor
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eme de compacit
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