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Volume 2008, Article ID 597241,12pages doi:10.1155/2008/597241

Research Article

A Perturbed Ostrowski-Type Inequality on

Time Scales for

k

Points for Functions Whose

Second Derivatives Are Bounded

Wenjun Liu,1Quoc Anh Ng ˆo,´ˆ 2, 3 and Wenbing Chen1

1College of Mathematics and Physics, Nanjing University of Information Science and Technology, Nanjing 210044, China

2Department of Mathematics, College of Science, Viet Nam National University, Hanoi, Vietnam

3Department of Mathematics, National University of Singapore, 2 Science Drive 2, Singapore 117543

Correspondence should be addressed to Wenjun Liu,[email protected]

Received 6 May 2008; Accepted 13 August 2008

Recommended by Kunquan Lan

We first derive a perturbed Ostrowski-type inequality on time scales forkpoints for functions whose second derivatives are bounded and then unify corresponding continuous and discrete versions. We also point out some particular perturbed integral inequalities on time scales for functions whose second derivatives are bounded as special cases.

Copyrightq2008 Wenjun Liu et al. 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

The following integral inequality which was first proved by Ostrowski in 1938 has received considerable attention from many researchers1–9.

Theorem 1.1. Let f : a, b → R be continuous on a, b and differentiable in a, b and its

derivativef : a, b → Ris bounded on a, b, that is, f∞ : supt∈a,b|fx| <. Then

for anyx∈a, b, the following inequality holds:

fx− 1

ba

b

a

ftdt

1 4

x−ab/22

b−a2

b−af. 1.1

The inequality is sharp in the sense that the constant1/4cannot be replaced by a smaller one.

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studied the theory of certain integral inequalities on time scales. For example, we refer the reader to 11–18. In 15, Bohner and Matthews established the following so-called Ostrowski inequality on time scales.

Theorem 1.2see15, Theorem 3.5. Leta, b, x, t∈T,a < b, andf:a, b → Rbe differentiable.

Then

b

a

tΔt−fxbaMh2x, a h2x, b, 1.2

wherehk·,·is defined byDefinition 2.9below andM supa<x<b|fΔx|.This inequality is sharp in the sense that the right-hand side of1.1cannot be replaced by a smaller one.

Liu and Ng ˆo then generalize the above Ostrowski inequality on time scales forkpoints

x1, x2, . . . , xk in19. They also extended the result by considering functions whose second

derivatives are bounded in20. They obtained the following theorem.

Theorem 1.3. Leta, b, x, t ∈ T,a < b, andf : a, b → Rbe a twice differentiable function on

a, bandfΔΔ:a, b → Rbounded, that is,M:supa<t<b|fΔΔx|<. Then

b

a

tΔt−xb−a h2x, a−h2x, bfΔx

Mh3x, a−h3x, b. 1.3

Theorem 1.3may be thought of as a perturbed version ofTheorem 1.2. In the present paper we will first derive a perturbed Ostrowski-type inequality on time scales for k

points x1, x2, . . . , xk for functions whose second derivatives are bounded and then unify corresponding continuous and discrete versions. We also point out some particular perturbed integral inequalities on time scales for functions whose second derivatives are bounded as special cases.

2. Time scales essentials

In this section, we briefly introduce the time scales theory and refer the reader to Hilger10 and the books21–23for further detailssee also19,20.

Definition 2.1. A time scaleTis an arbitrary nonempty closed subset of the real numbers.

Definition 2.2. Fort∈T, one defines theforward jump operatorσ:T → Tbyσt inf{s∈T:

s > t},while thebackward jump operatorρ:T → Tis defined byρt sup{s∈T:s < t}.

In this definition, we put inf∅ supT i.e.,σt t if T has a maximum tand sup∅infTi.e.,ρt tifThas a minimumt, where∅denotes the empty set. Ifσt> t, then we say thattisright-scattered, while ifρt< t, then we say thattisleft-scattered. Points that are right-scattered and left-scattered at the same time are called isolated. Ifσt tand

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Definition 2.3. Lett∈T, then two mappingsμ, ν:T → 0,∞satisfying

μt:σtt, νt:tρt 2.1

are called thegraininess functions.

We now introduce the setTκwhich is derived from the time scalesTas follows. IfT has a left-scattered maximumt, thenTκ : T− {t}, otherwiseTκ : T. Furthermore, for a

functionf:T → R, we define the function :T Rbyfσt fσtfor alltT.

Definition 2.4. Letf :T → Rbe a function on time scales. Then fort∈Tκ, one defines fΔt

to be the number, if one exists, such that for allε >0 there is a neighborhoodUoftsuch that for allsU

fσtfsfΔtσtsε|σts|. 2.2

We say thatfisΔ-differentiable onTκprovidedfΔtexists for alltTκ. We talk about the

second derivative fΔΔ providedfΔ is differentiable onTκ2

Tκκ with derivativefΔΔ Δ:Tκ2

→ R.

Definition 2.5. A mappingf :T → Ris calledrd-continuousdenoted byfCrdprovided

that it satisfies

1fis continuous at each right-dense point ofT;

2the left-sided limit limstfs ft−exists at each left-dense pointtofT.

Remark 2.6. It follows from Theorem 1.74 of Bohner and Peterson 21 that every

rd-continuous function has an antiderivative.

Definition 2.7. A functionF : T → Ris called aΔ-antiderivative off : T → Rprovided

FΔt ftholds for allt∈Tκ. Then theΔ-integral offis defined by

b

a

ftΔtFbFa. 2.3

Proposition 2.8. Letf, gbe rd-continuous,a, b, c∈T, andα, β∈R. Then

1abαft βgtΔtαabftΔtβabgtΔt,

2abftΔtbaftΔt,

3abftΔtacftΔtcbftΔt,

4abftgΔtΔt fgb−fga−abfΔtgσtΔt, 5aaftΔt0,

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Definition 2.9. Lethk:T2 R,kN

0be defined by

h0t, s 1 ∀s, t∈T 2.4

and then recursively by

hk1t, s t

s

hkτ, sΔτs, t∈T. 2.5

Remark 2.10. It follows fromProposition 2.86that ifst, thenhk1t, s≥0 for allt, s ∈T and allk∈N.

Remark 2.11. If we lethΔkt, sdenote for each fixedsthe derivative ofhkt, swith respect to

t, then

hΔkt, s hk−1t, s, fork∈N, t∈Tκ. 2.6

3. The perturbed Ostrowski inequality on time scales

Our main result reads as follows .

Theorem 3.1. Suppose that

1a, b ∈ T,Ik :a x0 < x1 < · · · < xk−1 < xk bis a division of the intervala, bfor

x0, x1, . . . , xk∈T;

2αi∈Ti0, . . . , k1is “k2” points so thatα0 a,αi ∈xi−1, xi i1, . . . , kand

αk1b;

3f : a, b → Ris a twice differentiable function ona, band fΔΔ : a, b → R is

bounded, that is,M:supa<t<b|fΔΔt|<.

Then

b

a

tΔt− k

i0

αi1−αifσxi

k−1

i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi

M k−1

i0

h3xi1, αi1−h3xi, αi1.

3.1

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Lemma 3.2generalized montgomery identity. Under the assumptions ofTheorem 3.1,

k

i0

αi1−αifσxi b

a

tΔt−

b

a

Kt, IkfΔΔΔt

k−1 i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi ,

3.2

where

Kt, Ik

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

h2t, α1, t∈a, x1,

h2t, α2, t∈x1, x2,

.. .

h2t, αk−1, t∈xk−2, xk−1,

h2t, αk, t∈xk−1, b.

3.3

Proof. Integrating by parts and applyingProposition 2.84, we have

b

a

Kt, IkfΔΔtΔt

k−1 i0

xi1

xi

Kt, IkfΔΔtΔt

k−1 i0

xi1

xi

h2t, αi1fΔΔtΔt

k−1 i0

αi1

xi

h2t, αi1fΔΔtΔt xi1

αi1

h2t, αi1fΔΔtΔt

k−1 i0

h2αi1, αi1fΔαi1−h2xi, αi1fΔxi− αi1

xi

fΔσthΔ2t, αi1Δt

h2xi1, αi1fΔxi1−h2αi1, αi1fΔαi1− xi1

αi1

fΔσthΔ2t, αi1Δt

k−1 i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi

αi1

xi

fΔσtt−αi1Δt− xi1

αi1

fΔσtt−αi1Δt

k−1 i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi xixi−αi1

αi1

x1

tΔt−xi1xi1−αi1 xi1

αi1

tΔt

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b

a

tΔt k−1

i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi aa−α1

k−1 i1

xix

iαi1−bb−αk

k−2

i0

x

i1xi1−αi1

b

a

tΔt− k

i0

xi1−αi

k−1

i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi ,

3.4

that is,3.2holds.

Proof ofTheorem 3.1. By applyingLemma 3.2, we get

b

a

tΔt− k

i0

αi1−αifσxi

k−1

i0

h2xi1, αi1fΔxi1−h2xi, αi1fΔxi

b

a

Kt, IkfΔΔtΔt

k−1

i0 xi1

xi

Kt, IkfΔΔtΔt

k−1

i0 xi1

xi

|Kt, Ik||fΔΔt|Δt≤M k−1

i0 xi1

xi

|h2t, αi1|Δt

M k−1

i0

αi1

xi

αi1

t

αi1−τΔτ

Δt

xi1

αi1

h2t, αi1Δt

M k−1

i0

αi1

xi

h2t, αi1Δt xi1

αi1

h2t, αi1Δt

M k−1

i0

h3xi1, αi1−h3xi, αi1.

3.5

The proof is complete.

If we apply the the inequality3.1to different time scales, we will get some well-known and some new results.

Corollary 3.3continuous case. LetTR. Then our delta integral is the usual Riemann integral

from calculus. Hence,

h2t, s t−s 2

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This leads us to state the following inequality:

b

a

ftΔtk

i0

αi1−αifxi 1 2

k−1

i0

xi1−αi12fxi1−xiαi12fxi

M 6

k−1

i0

xi1−αi13−xi−αi13 ,

3.7

whereMsupa<x<b|fx|.

Remark 3.4. The inequality 3.7is exactly the generalized Ostrowski inequality shown in

24.

Corollary 3.5discrete case. LetTZ,a0,bn. Suppose that

1Ik: 0j0< j1<· · ·< jk−1< jknis a division of0, n∩Zforj0, k1, . . . , jk∈Z; 2pi ∈Zi0, . . . , k1is “k2” points so thatp00,pi ∈ji−1, ji∩Zi1, . . . , k

andpk1n;

3fk xk.

Then,

n

j1

xjk

i0

pi1−pixji1

k−1

i0

h2ji1, pi1Δxji1−h2ji, pi1Δxji

M k−1

i0

h3ji1, pi1−h3ji, pi1

3.8

for alli1, n, where

M sup 1≤in−1

Δ2x

i, hkt, s

ts k

3.9

for allt, s∈Z.

Corollary 3.6quantum calculus case. LetTqN0,q >1,aqm, bqnwithm < n. Suppose

that

1Ik:qmqj0 < qj1 <· · ·< qjk−1 < qjk qnis a division ofqm, qnqN0forj0, j1, . . . , jk

N0;

2qpiqN0 i0, . . . , k1is “k2” points so thatqp0 qm,qpi ∈qji−1, qjiqN0 i

1, . . . , kandqpk1qm;

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Then,

qn

qm

fqtΔtk

i0

qpi1−qpifqji1

k−1 i0

h2qji1, qpi1

fqji11−fqji1 q−1qji1 −h2q

ji, qpifq

ji1−fqji

q−1qji

M k−1

i0

h3qji1, qpi1−h3qji, qpi1,

3.10

where

M sup

qm<t<qn

fq2t−qqq1f12qt t2 qft

, hkt, s k−1

ν0

ts

ν μ0

,t, sqN0.

3.11

4. Some particular perturbed integral inequalities on time scales

In this section, we point out some particular perturbed integral inequalities on time scales for functions whose second derivatives are bounded as special cases, such as perturbed rectangle inequality on time scales, perturbed trapezoid inequality on time scales, perturbed mid-point inequality on time scales, perturbed Simpson inequality on time scales, perturbed averaged mid-point-trapezoid inequality on time scales, and others. Throughout this section, we always assume thata, b∈Twitha > bandf :a, b → Ris differentiable. We denote

M sup

a<x<b

fΔΔx<. 4.1

Proposition 4.1. Suppose thatα ∈ a, b∩T. Then one has the perturbed rectangle inequality on

time scales

b

a

tΔt−α−afσa b−αfσb h2b, αfΔb−h2a, αfΔa

Mh3b, α−h3a, α.

4.2

Proof. We choosex0 a,x1 b,α0 a,α1 α∈a, bandα2 binTheorem 3.1to get the

result.

Remark 4.2. aIf we chooseαbin4.2, we get the perturbed left rectangle inequality on

time scales

b

a

tΔtbafσah

2a, bfΔa

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bIf we chooseαain4.2, we get the perturbed right rectangle inequality on time scales

b

a

tΔt−b−afσb h2b, afΔb

Mh3b, a. 4.4

cIf we chooseα ab/2 in4.2, we get the perturbed trapezoid inequality on time scales

b

a

tΔt−f

σa fσb

2 b−a

h2

b,ab

2

fΔb−h2

a,ab

2

fΔa

M

h3

b,ab

2

h3

a,ab

2

.

4.5

Proposition 4.3. Suppose thatx∈a, b∩T1∈a, x∩Tandα2∈x, b∩T. Then one has the

perturbed inequality on time scales

b

a

tΔt−α1−afσa α2−α1fσx b−α2fσb

h2x, α1fΔx−h2a, α1fΔa h2b, α2fΔb−h2x, α2fΔx

Mh3x, α1−h3a, α1 h3b, α2−h3x, α2.

4.6

Remark 4.4. If we choose α1 aandα2 binProposition 4.3, we get exactlyTheorem 1.3.

Therefore,Theorem 3.1is a generalization of Theorem 4 in20. If we choosex ab/2 in

3.1, we get the perturbed mid-point inequality on time scales

b

a

tΔt−

ab

2

b−a

h2

ab

2 , a

h2

ab

2 , b

fΔ

ab

2 ≤M h3

ab

2 , a

h3

ab

2 , b

.

4.7

Corollary 4.5. Suppose thatx∈5ab/6,a5b/6∩T1 5ab/6andα2 a5b/6.

Then one has the perturbed inequality on time scales

b

a

tΔt−ba

3

fσa fσb

2 2f

σx h2

x,5ab

6

fΔx−h2

a,5ab

6

fΔah2

b,a5b

6

fΔb−h2

x,a5b

6

fΔx

M

h3

x,5ab

6

h3

a,5ab

6

h3

b,a5b

6

h3

x,a5b

6

.

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Remark 4.6. If we choosex ab/2 in4.8, we get the perturbed Simpson inequality on time scales

b

a

tΔtba

3

a b

2 2f

σ

ab

2 h2

ab

2 , 5ab

6

fΔ

ab

2

h2

a,5ab

6

fΔa

h2

b,a5b

6

fΔb−h2

ab

2 ,

a5b

6

fΔ

ab

2 ≤M h3

ab

2 , 5ab

6

h3

a,5ab

6

h3

b,a5b

6

h3

ab

2 ,

a5b

6

.

4.9

Corollary 4.7. Suppose thatab/2∈T1 ∈a,ab/2∩Tandα2 ∈ab/2, b∩T.

Then one has the perturbed inequality on time scales

b

a

tΔt−

α1−afσa α2−α1fσ

ab

2

b−α2fσb

h2

ab

2 , α1

fΔ

ab

2

h2a, α1fΔa h2b, α2fΔb−h2

ab

2 , α2

fΔ

ab

2 ≤M h3

ab

2 , α1

h3a, α1 h3b, α2−h3

ab

2 , α2

.

4.10

Remark 4.8. If we chooseα1 3ab/4 andα2 a3b/4 in4.10, we get the perturbed

averaged mid-point-trapezoid inequality on time scales

b

a

tΔt−ba

2

fσa fσb

2 f

σ

ab

2 h2

ab

2 , 3ab

4

fΔ

ab

2

h2

a,3ab

4

fΔa

h2

b,a3b

4

fΔb−h2

ab

2 ,

a3b

4

fΔ

ab

2 ≤M h3

ab

2 , 3ab

4

h3

a,3ab

4

h3

b,a3b

4

h3

ab

2 ,

a3b

4

.

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Acknowledgments

The authors wish to express their gratitude to the anonymous referees for a number of valuable comments and suggestions. This work was supported by the Science Research Foundation of Nanjing University of Information Science and Technology.

References

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2 S. S. Dragomir, R. P. Agarwal, and P. Cerone, “On Simpson’s inequality and applications,”Journal of Inequalities and Applications, vol. 5, no. 6, pp. 533–579, 2000.

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