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Applied Mathematics Letters
journal homepage:www.elsevier.com/locate/aml
On the perturbation of Volterra integro-differential equations
Soon-Mo Jung
a, Sebaheddin Şevgin
b,∗, Hamdullah Şevli
caMathematics Section, College of Science and Technology, Hongik University, 339-701 Jochiwon, Republic of Korea
bYuzuncu Yil University, Faculty of Art and Science, Department of Mathematics, 65080 Van, Turkey
cDepartment of Mathematics, Faculty of Sciences and Arts, Istanbul Commerce University, 34672 Uskudar, Istanbul, Turkey
a r t i c l e i n f o
Article history:
Received 23 August 2012
Received in revised form 23 October 2012 Accepted 23 October 2012
Keywords:
Volterra integro-differential equation Volterra integral equation of the second
kind Perturbation Hyers–Ulam stability
Generalized Hyers–Ulam stability
a b s t r a c t
In this work, we will prove that every solution of a perturbed Volterra integro-differential equation can be approximated by a solution of the Volterra integro-differential equation.
© 2013 Elsevier Ltd. All rights reserved.
1. Introduction
Let I be either
(−∞,
b] ,
R, [
a, ∞)
, or a closed interval[
a,
b]
with−∞ <
a<
b< ∞
, let c be a fixed point of I, and letϕ :
I→ [
0, ∞)
be a continuous function.Recently, S.-M. Jung [1] proved that if a continuous function u
:
I→
C satisfies the perturbed Volterra integral equation of the second kind
u
(
t) −
t cF
(τ,
u(τ))
dτ
≤ ϕ(
t)
for all t
∈
I, then under some additional conditions, there exist a unique continuous function u0:
I→
C and a constant C>
0 such thatu0
(
t) =
t cF
(τ,
u0(τ))
dτ
and|
u(
t) −
u0(
t)| ≤
Cϕ(
t)
for all t∈
I.In this work, we will investigate the solutions u
:
I→
R of the integro-differential inequality
u′
(
t) +
p(
t)
u(
t) +
q(
t) +
t cK
(
t, τ)
u(τ)
dτ
≤ ϕ(
t)
(1.1)∗Corresponding author. Tel.: +90 5055938215; fax: +90 4322251806.
E-mail addresses:smjung@hongik.ac.kr(S.-M. Jung),ssevgin@yahoo.com,ssevgin@yyu.edu.tr(S. Şevgin),hsevli@yahoo.com(H. Şevli).
0893-9659/$ – see front matter©2013 Elsevier Ltd. All rights reserved.
doi:10.1016/j.aml.2012.10.018
which is the perturbed form of the Volterra integro-differential equation
u′
(
t) +
g(
t)
u(
t) +
h(
t) +
t cK
(
t, τ)
u(τ)
dτ =
0.
(1.2)More precisely, we will prove that if p
:
I→
R,
q:
I→
R,
K:
I×
I→
R andϕ :
I→ [
0, ∞)
are sufficiently smooth functions and if a continuously differentiable function u:
I→
R satisfies the perturbed Volterra integro-differential equation(1.1)for all t∈
I, then there exists a unique solution u0:
I→
R of the Volterra integro-differential equation(1.2) such that|
u(
t) −
u0(
t)| ≤
exp
−
t cp
(τ)
dτ
b tϕ(ξ)
exp
ξ cp
(τ)
dτ
dξ
for all t∈
I (provided that I= (−∞,
b]
or[
a,
b]
).2. The main results
In the following theorem, we will investigate the perturbation problem of the Volterra integro-differential equation(1.2) by using ideas from [1–3]. More precisely, we provide a characterization of the integro-differential inequality(1.1)for the class of real-valued functions.
Theorem 2.1. Let I
= [
a,
b]
for given real numbers a,
b with a<
b and let c∈
I. Assume that p:
I→
R,
q:
I→
R, and K:
I×
I→
R are continuous functions such that p(
t)
and exp
tcp
(τ)
dτ
q(
t)
are integrable on(
c,
d)
for each d∈
I with d>
c. Moreover, supposeϕ :
I→ [
0, ∞)
is a function such thatϕ(
t)
exp
tcp
(τ)
dτ
is integrable on I. If a continuously differentiable function u:
I→
R satisfies the integro-differential inequality(1.1)for all t∈
I, then there exists a uniqueα ∈
R such that
u
(
t) − α
exp
−
t cp
(τ)
dτ
+
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξc
p
(τ)
dτ
dξ +
exp
−
t cp
(τ)
dτ
t c
ξc
K
(ξ, τ)
u(τ)
dτ
exp
ξc
p
(τ)
dτ
dξ
≤
exp
−
t cp
(τ)
dτ
b tϕ(ξ)
exp
ξc
p
(τ)
dτ
d
ξ
(2.1)for every t
∈
I.Proof. We will now introduce an auxiliary function z
:
I→
R defined by z(
t) :=
exp
tc
p
(τ)
dτ
u
(
t) +
t cq
(ξ)
exp
ξc
p
(τ)
dτ
dξ +
t c
ξ cK
(ξ, τ)
u(τ)
dτ
exp
ξ cp
(τ)
dτ
dξ
for every t
∈
I. By the fundamental theorem of calculus and in view of(1.1), we get|
z(
t) −
z(
s)| =
exp
t cp
(τ)
dτ
u
(
t) −
exp
s cp
(τ)
dτ
u(
s) +
t s
q(ξ) +
ξc
K
(ξ, τ)
u(τ)
dτ
exp
ξ cp
(τ)
dτ
dξ
=
t sd d
ξ
exp
ξc
p
(τ)
dτ
u(ξ)
dξ +
t s
q
(ξ) +
ξc
K
(ξ, τ)
u(τ)
dτ
exp
ξc
p
(τ)
dτ
dξ
=
t sexp
ξc
p
(τ)
dτ
u′
(ξ) +
p(ξ)
u(ξ) +
q(ξ) +
ξc
K
(ξ, τ)
u(τ)
dτ
dξ
≤
t sϕ(ξ)
exp
ξc
p
(τ)
dτ
dξ
(2.2)
for any s
,
t∈
I.Since
ϕ(
t)
exp
tc p
(τ)
dτ
is assumed to be integrable on I, the inequality(2.2)implies that for any givenε >
0 there exists a t0∈
I such that s,
t≥
t0implies|
z(
t) −
z(
s)| ≤ ε
. Indeed,{
z(
s)}
s∈Iis a Cauchy net and hence there exists a real numberα
such that z(
s) → α
as s→
b, since R is complete.Finally, it follows from(2.2)and the above argument that for any t
∈
I,
u
(
t) − α
exp
−
t cp
(τ)
dτ
+
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξc
p
(τ)
dτ
dξ +
exp
−
t cp
(τ)
dτ
t c
ξc
K
(ξ, τ)
u(τ)
dτ
exp
ξc
p
(τ)
dτ
dξ
=
exp
−
t cp
(τ)
dτ
(
z(
t) − α)
≤
exp
−
t cp
(τ)
dτ
|
z(
t) −
z(
s)| +
exp
−
t cp
(τ)
dτ
|
z(
s) − α|
≤
exp
−
t cp
(τ)
dτ
t sϕ(ξ)
exp
ξc
p
(τ)
dτ
dξ
+
exp
−
t cp
(τ)
dτ
|
z(
s) − α|
→
exp
−
t cp
(τ)
dτ
t bϕ(ξ)
exp
ξc
p
(τ)
dτ
dξ
as s
→
b,
since we assumed that z(
s) → α
as s→
b, which proves the validity of(2.1).It now remains to prove the uniqueness of
α
. Assume thatβ ∈
R also satisfies the inequality(2.1)in place ofα
. Then, we have
exp
−
t cp
(τ)
dτ
(β − α)
≤
2 exp
−
t cp
(τ)
dτ
b tϕ(ξ)
exp
ξc
p
(τ)
dτ
dξ
for any t∈
I. It follows from the integrability hypotheses that| β − α| ≤
2
b tϕ(ξ)
exp
ξ cp
(τ)
dτ
d
ξ →
0 as t→
b.
This implies the uniqueness ofα
.Remark 2.1. It is not difficult to show that for any real number
α
, u(
t) = α
exp
−
t cp
(τ)
dτ
−
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξc
p
(τ)
dτ
dξ
−
exp
−
t cp
(τ)
dτ
t c
ξc
K
(ξ, τ)
u(τ)
dτ
exp
ξc
p
(τ)
dτ
dξ
is the general solution of the Volterra integro-differential equation(1.2), where
α
is an arbitrary real number.In the preceding theorem, we have investigated the perturbed Volterra integro-differential equation(1.2)defined on a bounded and closed interval. We will now prove the theorem for the case of unbounded intervals. More precisely, Theorem 2.1is also true if I is replaced by an unbounded interval such as
[
a, ∞)
. We can prove the following theorem by replacing b with∞
in the proof ofTheorem 2.1. Hence, we omit the proof.Theorem 2.2. For any given real number a, let I
= [
a, ∞)
and c be a fixed point of I. Assume that p:
I→
R,
q:
I→
R, and K:
I×
I→
R are continuous functions such that p(
t)
and exp
tc p
(τ)
dτ
q(
t)
are integrable on(
c,
d)
for each d∈
I with d>
c. Moreover, supposeϕ :
I→ [
0, ∞)
is a function such thatϕ(
t)
exp
tc p
(τ)
dτ
is integrable on I. If a continuously differentiable function u:
I→
R satisfies the integro-differential inequality(1.1)for all t∈
I, then there exists a uniqueα ∈
R such that
u
(
t) − α
exp
−
t cp
(τ)
dτ
+
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξc
p
(τ)
dτ
dξ +
exp
−
t cp
(τ)
dτ
t c
ξc
K
(ξ, τ)
u(τ)
dτ
exp
ξc
p
(τ)
dτ
dξ
≤
exp
−
t cp
(τ)
dτ
∞ tϕ(ξ)
exp
ξc
p
(τ)
dτ
dξ
for any t∈
I.Applying an idea from [3] and usingTheorem 2.2, we can proveTheorem 2.1for the case of I
=
R.Corollary 2.3. Let c be a fixed real number. Assume that p
:
R→
R,
q:
R→
R, and K:
R×
R→
R are continuous functions such that p(
t)
and exp
tc p
(τ)
dτ
q(
t)
are integrable on(
c,
d)
for each d∈
R with d>
c. Moreover, supposeϕ :
R→ [
0, ∞)
is a function such thatϕ(
t)
exp
tc p
(τ)
dτ
is integrable on R. If a continuously differentiable function u:
R→
R satisfies the integro-differential inequality(1.1)for all t∈
R, then there exists a uniqueα ∈
R such that
u
(
t) − α
exp
−
t cp
(τ)
dτ
+
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξ cp
(τ)
dτ
dξ +
exp
−
t cp
(τ)
dτ
t c
ξ cK
(ξ, τ)
u(τ)
dτ
exp
ξ cp
(τ)
dτ
dξ
≤
exp
−
t cp
(τ)
dτ
∞ tϕ(ξ)
exp
ξ cp
(τ)
dτ
d
ξ
(2.3)for all t
∈
R.Proof. For any n
∈
N0, we define In= [
c−
n, ∞)
. According toTheorem 2.2, there exists a uniqueα
n∈
R such that
u
(
t) − α
nexp
−
t cp
(τ)
dτ
+
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξ cp
(τ)
dτ
dξ +
exp
−
t cp
(τ)
dτ
t c
ξ cK
(ξ, τ)
u(τ)
dτ
exp
ξ cp
(τ)
dτ
dξ
≤
exp
−
t cp
(τ)
dτ
∞t
ϕ(ξ)
exp
ξc
p
(τ)
dτ
d
ξ
(2.4)for any t
∈
In. The uniqueness ofα
nimplies that if t∈
In, thenα
n= α
n+1= α
n+2= · · · .
In general, we conclude that
α
0= α
1= α
2= · · · = α
n= · · · =: α.
(2.5)Consequently, the validity of(2.3)follows from(2.4)and(2.5)because for each t
∈
R, there exists an n∈
N0with t∈
In. The uniqueness ofα
can be proved by applying the same argument as was given in the proof ofTheorem 2.1.If we set K
(
t,
s) ≡
0 inCorollary 2.3, then we obtain the generalized Hyers–Ulam stability of the first-order linear differential equations, u′(
t) +
p(
t)
u(
t) +
q(
t) =
0 (cf. [4,5] and refer to [6–11] for the definition of Hyers–Ulam stability).In the following corollary, we will deal with the case of I
=
R only.Corollary 2.4. Let c be a fixed real number. Assume that p
:
R→
R and q:
R→
R are continuous functions such that p(
t)
and exp
tcp
(τ)
dτ
q(
t)
are integrable on(
c,
d)
for each d∈
R with d>
c. Moreover, supposeϕ :
R→ [
0, ∞)
is a function such thatϕ(
t)
exp
tc p
(τ)
dτ
is integrable on R. If a continuously differentiable function u:
R→
R satisfies the differential inequality|
u′(
t) +
p(
t)
u(
t) +
q(
t)| ≤ ϕ(
t)
for all t
∈
R, then there exists a uniqueα ∈
R such that
u
(
t) − α
exp
−
t cp
(τ)
dτ
+
exp
−
t cp
(τ)
dτ
t cq
(ξ)
exp
ξc
p
(τ)
dτ
dξ
≤
exp
−
t cp
(τ)
dτ
∞ tϕ(ξ)
exp
ξc
p
(τ)
dτ
dξ
for all t∈
R.Acknowledgments
This research was completed with the support of The Scientific and Technological Research Council of Turkey while the first author was a visiting scholar at Istanbul Commerce University, Istanbul, Turkey.
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