Báo cáo hóa học: " Research Article A Perturbed Ostrowski-Type Inequality on Time Scales for k Points for Functions Whose Second Derivatives Are Bounded" doc

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Báo cáo hóa học: " Research Article A Perturbed Ostrowski-Type Inequality on Time Scales for k Points for Functions Whose Second Derivatives Are Bounded" doc

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Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2008, Article ID 597241, 12 pages 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, 1 Qu ´ ˆoc Anh Ng ˆ o, 2, 3 and Wenbing Chen 1 1 College of Mathematics and Physics, Nanjing University of Information Science and Technology, Nanjing 210044, China 2 Department of Mathematics, College of Science, Viet Nam National University, Hanoi, Vietnam 3 Department of Mathematics, National University of Singapore, 2 Science Drive 2, Singapore 117543 Correspondence should be addressed to Wenjun Liu, wjliu@nuist.edu.cn Received 6 May 2008; Accepted 13 August 2008 Recommended by Kunquan Lan We first derive a perturbed Ostrowski-type inequality on time scales for k points 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. Copyright q 2008 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 researchers 1–9. Theorem 1.1. Let f : a, b → R be continuous on a, b and differentiable in a, b and its derivative f  : a, b → R is bounded on a, b, that is, f   ∞ : sup t∈a,b |f  x| < ∞.Then for any x ∈ a, b, the following inequality holds:     fx − 1 b − a  b a ftdt     ≤  1 4  x − a  b/2 2 b − a 2  b − af   ∞ . 1.1 The inequality is sharp in the sense that the constant 1/4 cannot be replaced by a smaller one. In 1988, Hilger 10 developed the theory of time scales as a theory capable to contain both difference and differential calculus in a consistent way. Since then, many authors have 2 Journal of Inequalities and Applications 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 1.2 see 15, Theorem 3.5. Let a, b, x, t ∈ T, a<b, and f : a, b → R be differentiable. Then      b a f σ tΔt − fxb − a     ≤ Mh 2 x, ah 2 x, b, 1.2 where h k ·, · is defined by Definition 2.9 below and M  sup a<x<b |f Δ x|. This inequality is sharp in the sense that the right-hand side of 1.1 cannot be replaced by a smaller one. Liu and Ng ˆ o then generalize the above Ostrowski inequality on time scales for k points x 1 ,x 2 , ,x k in 19. They also extended the result by considering functions whose second derivatives are bounded in 20. They obtained the following theorem. Theorem 1.3. Let a, b, x, t ∈ T, a<b, and f : a, b → R be a twice differentiable function on a, b and f ΔΔ : a, b → R bounded, that is, M : sup a<t<b |f ΔΔ x| < ∞.Then      b a f σ tΔt − f σ xb − ah 2 x, a − h 2 x, bf Δ x     ≤ Mh 3 x, a − h 3 x, b. 1.3 Theorem 1.3 may be thought of as a perturbed version of Theorem 1.2. In the present paper we will first derive a perturbed Ostrowski-type i nequality on time scales for k points x 1 ,x 2 , ,x k 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 Hilger 10 and the books 21–23 for further details see also 19, 20. Definition 2.1. A time scale T is an arbitrary nonempty closed subset of the real numbers. Definition 2.2. For t ∈ T, one defines the forward jump operator σ : T → T by σtinf{s ∈ T : s>t}, while the backward jump operator ρ : T → T is defined by ρtsup{s ∈ T : s<t}. In this definition, we put inf ∅  sup T i.e., σtt if T has a maximum t and sup ∅  inf T i.e., ρt t if T has a minimum t, where ∅ denotes the empty set. If σt >t, then we say that t is right-scattered, while if ρt <t, then we say that t is left-scattered.Points that are right-scattered and left-scattered at the same time are called isolated. If σtt and t<sup T, then t is called right dense,andifρtt and t>inf T, then t is called left dense. Points that are both right dense and left dense are called dense. Wenjun Liu et al. 3 Definition 2.3. Let t ∈ T, then two mappings μ, ν : T → 0, ∞ satisfying μt : σt − t, νt : t − ρt2.1 are called the graininess functions. We now introduce the set T κ which is derived from the time scales T as follows. If T has a left-scattered maximum t, then T κ : T −{t}, otherwise T κ : T. Furthermore, for a function f : T → R, we define the function f σ : T → R by f σ tfσt for all t ∈ T. Definition 2.4. Let f : T → R be a function on time scales. Then for t ∈ T κ , one defines f Δ t to be the number, if one exists, such that for all ε>0 there is a neighborhood U of t such that for all s ∈ U   f σ t − fs − f Δ tσt − s   ≤ ε|σt − s|. 2.2 We say that f is Δ-differentiable on T κ provided f Δ t exists for all t ∈ T κ . We talk about the second derivative f ΔΔ provided f Δ is differentiable on T κ 2 T κ  κ with derivative f ΔΔ  f Δ  Δ : T κ 2 → R. Definition 2.5. A mapping f : T → R is called rd-continuous denoted by f ∈ C rd  provided that it satisfies 1 f is continuous at each right-dense point of T; 2 the left-sided limit lim s → t− fsft− exists at each left-dense point t of T. 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 function F : T → R is called a Δ-antiderivative of f : T → R provided F Δ tft holds for all t ∈ T κ . Then the Δ-integral of f is defined by  b a ftΔt  Fb − Fa. 2.3 Proposition 2.8. Let f, g be rd-continuous, a, b, c ∈ T, and α, β ∈ R.Then 1  b a αftβgtΔt  α  b a ftΔt  β  b a gtΔt, 2  b a ftΔt  −  a b ftΔt, 3  b a ftΔt   c a ftΔt   b c ftΔt, 4  b a ftg Δ tΔt fgb − fga −  b a f Δ tgσtΔt, 5  a a ftΔt  0, 6 If ft ≥ 0 for all a ≤ t<bthen  b a ftΔt ≥ 0. 4 Journal of Inequalities and Applications Definition 2.9. Let h k : T 2 → R, k ∈ N 0 be defined by h 0 t, s1 ∀s, t ∈ T 2.4 and then recursively by h k1 t, s  t s h k τ,sΔτ ∀s, t ∈ T. 2.5 Remark 2.10. It follows from Proposition 2.86 that if s ≤ t, then h k1 t, s ≥ 0 for all t, s ∈ T and all k ∈ N. Remark 2.11. If we let h Δ k t, s denote for each fixed s the derivative of h k t, s with respect to t, then h Δ k t, sh k−1 t, s, for k ∈ N,t∈ T κ . 2.6 3. The perturbed Ostrowski inequality on time scales Our main result reads as follows . Theorem 3.1. Suppose that 1 a, b ∈ T, I k : a  x 0 <x 1 < ··· <x k−1 <x k  b is a division of the interval a, b for x 0 ,x 1 , ,x k ∈ T; 2 α i ∈ T i  0, ,k 1 is “k  2” points so that α 0  a, α i ∈ x i−1 ,x i i  1, ,k and α k1  b; 3 f : a, b → R is a twice differentiable function on a, b and f ΔΔ : a, b → R is bounded, that is, M : sup a<t<b |f ΔΔ t| < ∞. Then       b a f σ tΔt − k  i0 α i1 − α i f σ x i  k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i        ≤ M k−1  i0 h 3 x i1 ,α i1  − h 3 x i ,α i1 . 3.1 To prove Theorem 3.1, we need the following generalized montgomery identity for twice differentiable function. This is motivated by the ideas of Sofo and Dragomir in 24, where the continuous version of a perturbed Ostrowski inequality for twice differentiable mappings was proved. Wenjun Liu et al. 5 Lemma 3.2 generalized montgomery identity. Under the assumptions of Theorem 3.1, k  i0 α i1 − α i f σ x i   b a f σ tΔt −  b a Kt, I k f ΔΔ Δt  k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i   , 3.2 where Kt, I k  ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ h 2 t, α 1 ,t∈ a, x 1 , h 2 t, α 2 ,t∈ x 1 ,x 2 , . . . h 2 t, α k−1 ,t∈ x k−2 ,x k−1 , h 2 t, α k ,t∈ x k−1 ,b. 3.3 Proof. Integrating by parts and applying Proposition 2.84 , we have  b a Kt, I k f ΔΔ tΔt  k−1  i0  x i1 x i Kt, I k f ΔΔ tΔt  k−1  i0  x i1 x i h 2 t, α i1 f ΔΔ tΔt  k−1  i0   α i1 x i h 2 t, α i1 f ΔΔ tΔt   x i1 α i1 h 2 t, α i1 f ΔΔ tΔt   k−1  i0  h 2 α i1 ,α i1 f Δ α i1  − h 2 x i ,α i1 f Δ x i  −  α i1 x i f Δ σth Δ 2 t, α i1 Δt  h 2 x i1 ,α i1 f Δ x i1  − h 2 α i1 ,α i1 f Δ α i1  −  x i1 α i1 f Δ σth Δ 2 t, α i1 Δt   k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i  −  α i1 x i f Δ σtt − α i1 Δt −  x i1 α i1 f Δ σtt − α i1 Δt   k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i f σ x i x i − α i1    α i1 x 1 f σ tΔt − f σ x i1 x i1 − α i1   x i1 α i1 f σ tΔt  6 Journal of Inequalities and Applications   b a f σ tΔt  k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i    f σ aa − α 1   k−1  i1 f σ x i x i − α i1  − f σ bb − α k  − k−2  i0 f σ x i1 x i1 − α i1    b a f σ tΔt − k  i0 f σ x i α i1 − α i  k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i   , 3.4 that is, 3.2 holds. Proof of Theorem 3.1. By applying Lemma 3.2,weget       b a f σ tΔt − k  i0 α i1 − α i f σ x i  k−1  i0  h 2 x i1 ,α i1 f Δ x i1  − h 2 x i ,α i1 f Δ x i              b a Kt, I k f ΔΔ tΔt           k−1  i0  x i1 x i Kt, I k f ΔΔ tΔt      ≤ k−1  i0  x i1 x i |Kt, I k ||f ΔΔ t|Δt ≤ M k−1  i0  x i1 x i |h 2 t, α i1 |Δt  M k−1  i0   α i1 x i   α i1 t α i1 − τΔτ  Δt   x i1 α i1 h 2 t, α i1 Δt   M k−1  i0   α i1 x i h 2 t, α i1 Δt   x i1 α i1 h 2 t, α i1 Δt   M k−1  i0 h 3 x i1 ,α i1  − h 3 x i ,α i1 . 3.5 The proof is complete. If we apply the the inequality 3.1 to different time scales, we will get some well- known and some new results. Corollary 3.3 continuous case. Let T  R. Then our delta integral is the usual Riemann integral from calculus. Hence, h 2 t, s t − s 2 2 , ∀t, s ∈ R. 3.6 Wenjun Liu et al. 7 This leads us to state the following inequality:       b a ftΔt − k  i0 α i1 − α i fx i  1 2 k−1  i0  x i1 − α i1  2 f  x i1  − x i − α i1  2 f  x i        ≤ M 6 k−1  i0  x i1 − α i1  3 − x i − α i1  3  , 3.7 where M  sup a<x<b |f  x|. Remark 3.4. The inequality 3.7 is exactly the generalized Ostrowski inequality shown in 24. Corollary 3.5 discrete case. Let T  Z, a  0, b  n. Suppose that 1 I k :0 j 0 <j 1 < ··· <j k−1 <j k  n is a division of 0,n ∩ Z for j 0 ,k 1 , ,j k ∈ Z; 2 p i ∈ Z i  0, ,k 1 is “k  2” points so that p 0  0, p i ∈ j i−1 ,j i  ∩ Z i  1, ,k and p k1  n; 3 fkx k . Then,      n  j1 x j − k  i0 p i1 − p i x j i 1  k−1  i0  h 2 j i1 ,p i1 Δx j i 1 − h 2 j i ,p i1 Δx j i       ≤ M k−1  i0 h 3 j i1 ,p i1  − h 3 j i ,p i1  3.8 for all i  1,n,where M  sup 1≤i≤n−1   Δ 2 x i   ,h k t, s  t − s k  3.9 for all t, s ∈ Z. Corollary 3.6 quantum calculus case. Let T  q N 0 , q>1, a  q m ,b q n with m<n. Suppose that 1 I k : q m  q j 0 <q j 1 < ···<q j k−1 <q j k  q n is a division of q m ,q n  ∩ q N 0 for j 0 ,j 1 , ,j k ∈ N 0 ; 2 q p i ∈ q N 0 i  0, ,k 1 is “k  2” points so that q p 0  q m , q p i ∈ q j i−1 ,q j i  ∩ q N 0 i  1, ,k and q p k1  q m ; 3 f : q m ,q n  → R is differentiable. 8 Journal of Inequalities and Applications Then,       q n q m fqtΔt − k  i0 q p i1 − q p i fq j i 1   k−1  i0  h 2 q j i1 ,q p i1  fq j i1 1  − fq j i1  q − 1q j i1 − h 2 q j i ,q p i  fq j i 1  − fq j i  q − 1q j i       ≤ M k−1  i0 h 3 q j i1 ,q p i1  − h 3 q j i ,q p i1 , 3.10 where M  sup q m <t<q n     fq 2 t − q  1fqtqft qq − 1 2 t 2     ,h k t, s k−1  ν0 t − q ν s  ν μ0 q μ , ∀t, s ∈ q N 0 . 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 that a, b ∈ T with a>band f : a, b → R is differentiable. We denote M  sup a<x<b   f ΔΔ x   < ∞. 4.1 Proposition 4.1. Suppose that α ∈ a, b ∩ T. Then one has the perturbed rectangle inequality on time scales      b a f σ tΔt − α − af σ ab − αf σ b   h 2 b, αf Δ b − h 2 a, αf Δ a      ≤ Mh 3 b, α − h 3 a, α. 4.2 Proof. We choose x 0  a, x 1  b, α 0  a, α 1  α ∈ a, b and α 2  b in Theorem 3.1 to get the result. Remark 4.2. a If we choose α  b in 4.2, we get the perturbed left rectangle inequality on time scales      b a f σ tΔt − b − af σ a − h 2 a, bf Δ a     ≤−Mh 3 a, b. 4.3 Wenjun Liu et al. 9 b If we choose α  a in 4.2, we get the perturbed right rectangle inequality on time scales      b a f σ tΔt − b − af σ bh 2 b, af Δ b     ≤ Mh 3 b, a. 4.4 c If we choose α a  b/2in4.2, we get the perturbed trapezoid inequality on time scales      b a f σ tΔt − f σ af σ b 2 b − a  h 2  b, a  b 2  f Δ b − h 2  a, a  b 2  f Δ a      ≤ M  h 3  b, a  b 2  − h 3  a, a  b 2  . 4.5 Proposition 4.3. Suppose that x ∈ a, b ∩ T, α 1 ∈ a, x ∩ T and α 2 ∈ x, b ∩ T. Then one has the perturbed inequality on time scales      b a f σ tΔt −  α 1 − af σ aα 2 − α 1 f σ xb − α 2 f σ b    h 2 x, α 1 f Δ x − h 2 a, α 1 f Δ ah 2 b, α 2 f Δ b − h 2 x, α 2 f Δ x      ≤ Mh 3 x, α 1  − h 3 a, α 1 h 3 b, α 2  − h 3 x, α 2 . 4.6 Remark 4.4. If we choose α 1  a and α 2  b in Proposition 4.3, we get exactly Theorem 1.3. Therefore, Theorem 3.1 is a generalization of Theorem 4 in 20. If we choose x a  b/2in 3.1, we get the perturbed mid-point inequality on time scales      b a f σ tΔt − f σ  a  b 2  b − a  h 2  a  b 2 ,a  − h 2  a  b 2 ,b  f Δ  a  b 2      ≤ M  h 3  a  b 2 ,a  − h 3  a  b 2 ,b  . 4.7 Corollary 4.5. Suppose that x ∈ 5a b/6, a  5b/6 ∩ T, α 1 5a b/6 and α 2 a5b/6. Then one has the perturbed inequality on time scales      b a f σ tΔt − b − a 3  f σ af σ b 2  2f σ x    h 2  x, 5ab 6  f Δ x−h 2  a, 5a  b 6  f Δ ah 2  b, a  5b 6  f Δ b−h 2  x, a  5b 6  f Δ x      ≤ M  h 3  x, 5a  b 6  − h 3  a, 5a  b 6   h 3  b, a  5b 6  − h 3  x, a  5b 6  . 4.8 10 Journal of Inequalities and Applications Remark 4.6. If we choose x a  b/2in4.8, we get the perturbed Simpson inequality on time scales      b a f σ tΔt − b − a 3  f σ af σ b 2  2f σ  a  b 2    h 2  a  b 2 , 5a  b 6  f Δ  a  b 2  − h 2  a, 5a  b 6  f Δ a  h 2  b, a  5b 6  f Δ b − h 2  a  b 2 , a  5b 6  f Δ  a  b 2      ≤ M  h 3  a  b 2 , 5a  b 6  − h 3  a, 5a  b 6   h 3  b, a  5b 6  − h 3  a  b 2 , a  5b 6  . 4.9 Corollary 4.7. Suppose that a  b/2 ∈ T, α 1 ∈ a, a  b/2 ∩ T and α 2 ∈ a  b/2,b ∩ T. Then one has the perturbed inequality on time scales      b a f σ tΔt −  α 1 − af σ aα 2 − α 1 f σ  a  b 2  b − α 2 f σ b    h 2  a  b 2 ,α 1  f Δ  a  b 2  − h 2 a, α 1 f Δ ah 2 b, α 2 f Δ b − h 2  a  b 2 ,α 2  f Δ  a  b 2      ≤ M  h 3  a  b 2 ,α 1  − h 3 a, α 1 h 3 b, α 2  − h 3  a  b 2 ,α 2  . 4.10 Remark 4.8. If we choose α 1 3a  b/4andα 2 a  3b/4in4.10, we get the perturbed averaged mid-point-trapezoid inequality on time scales      b a f σ tΔt − b − a 2  f σ af σ b 2  f σ  a  b 2    h 2  a  b 2 , 3a  b 4  f Δ  a  b 2  − h 2  a, 3a  b 4  f Δ a  h 2  b, a  3b 4  f Δ b − h 2  a  b 2 , a  3b 4  f Δ  a  b 2      ≤ M  h 3  a  b 2 , 3a  b 4  − h 3  a, 3a  b 4   h 3  b, a  3b 4  − h 3  a  b 2 , a  3b 4  . 4.11 [...]... scales for functions whose second ˆ derivatives are bounded,” to appear in Inequality Theory and Applications, vol 6, 2009 21 M Bohner and A Peterson, Dynamic Equations on Time Scales: An Introduction with Application, Birkh¨ user, Boston, Mass, USA, 2001 a 12 Journal of Inequalities and Applications 22 M Bohner and A Peterso, Eds., Advances in Dynamic Equations on Time Scales, Birkh¨ user, Boston, a Mass,... 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Equations on Time Scales, Birkh ¨ auser, Boston, Mass, USA, 2003. 23 V. Lakshmikantham, S. Sivasundaram, and B. Kaymakcalan, Dynamic Systems on Measure Chains, vol. 370 of Mathematics and Its Applications,. 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. type inequality on time scales for functions whose second derivatives are bounded,” to appear in Inequality Theory and Applications, vol. 6, 2009. 21 M. Bohner and A. Peterson, Dynamic Equations

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