Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2012, Article ID 917120, 7 pages doi:10.1155/2012/917120 Research Article Optimal Bounds for Seiffert Mean in terms of One-Parameter Means Hua-Nan Hu,1 Guo-Yan Tu,2 and Yu-Ming Chu3 1 Acquisitions & Cataloging Department of Library, Huzhou Teachers College, Huzhou 313000, China Department of Basic Course Teaching, Tongji Zhejiang College, Jiaxing 314000, China 3 Department of Mathematics, Huzhou Teachers College, Huzhou 313000, China 2 Correspondence should be addressed to Yu-Ming Chu, chuyuming2005@yahoo.com.cn Received 11 July 2012; Accepted 7 September 2012 Academic Editor: Francisco J. Marcellán Copyright q 2012 Hua-Nan Hu 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. The authors present the greatest value r1 and the least value r2 such that the double inequality Jr1 a, b < T a, b < Jr2 a, b holds for all a, b > 0 with a / b, where T a, b and Jp a, b denote the Seiffert and pth one-parameter means of two positive numbers a and b, respectively. 1. Introduction For p ∈ R the pth one-parameter mean Jp a, b and the Seiffert mean T a, b of two positive real numbers a and b are defined by ⎧ ⎪ p ap1 − bp1 ⎪ ⎪ , p ⎪ ⎪ p ⎪ ⎪ ⎪ p 1 a − b ⎪ ⎪ ⎪ a−b ⎪ ⎨ , Jp a, b log a − log b ⎪ ⎪ ⎪ ⎪ ⎪ ab log a − log b ⎪ ⎪ ⎪ , ⎪ ⎪ a−b ⎪ ⎪ ⎩a, ⎧ ⎨ a/ b, p / 0, −1, a/ b, p 0, 1.1 a/ b, p −1, a b, a−b , T a, b 2 arctana − b/a b ⎩ a, a/ b, a b, 1.2 2 Journal of Applied Mathematics respectively. Recently, both mean values have been the subject of intensive research. In particular, many remarkable inequalities and properties for Jp and T can be found in the literature 1–14. It is well known that the one-parameter mean Jp a, b is continuous and strictly increasing with respect to p ∈ R for fixed a, b > 0 with a / b. Many mean values are the special case of the one-parameter mean, for example: a b , J1 a, b 2 √ a ab b , J1/2 a, b √3 J−1/2 a, b ab, 2ab J−2 a, b , a b the arithmetic mean, the Heronian mean, 1.3 the geometric mean, the harmonic mean. Seiffert 4 proved that the double inequality M1 a, b < T a, b < M2 a, b 1.4 √ holds for all a, b > 0 with a / b, where Mr a, b ar br /21/r r / 0 and M0 a, b ab is the rth power mean of a and b. In 15–17, the authors presented the best possible bounds for the Seiffert mean in terms of the Lehmer, power-type Heron, and one-parameter Gini means as follows: L0 a, b < T a, b < L1/3 a, b, Hlog 3/ logπ/2 a, b < T a, b < H5/2 a, b, 1.5 S1 a, b < T a, b < S5/3 a, b. for all a, b > 0 with a Lr a, b ar1 br1 /ar br , Hk a, b ak abk/2 / b, where √ 1/k 1/α−2 k α b /3 k / 0 and H0 a, b ab, and Sα a, b aα−1 bα−1 /a b / 2 and 1/ab denote the Lehmer, power-type Heron, and one-parameter Gini means S2 a, b aa bb of a and b, respectively. The purpose of this paper is to answer the question: what are the greatest value r1 and the least value r2 such that the double inequality Jr1 a, b < T a, b < Jr2 a, b holds for all a, b > 0 with a / b? 2. Lemma In order to establish our main result we need the following lemma. 1.6 Journal of Applied Mathematics 3 Lemma 2.1. If p 2/π − 2 1.75 · · · , t ≥ 1 and gt −p − 1t2p2 p 1t2p pp 1tp3 − 2p 12 tp2 2pp 3tp1 − 2p 12 tp pp 1tp−1 p 1t2 − p − 1, then there exists λ ∈ 1, ∞ such that gt > 0 for t ∈ 1, λ and gt < 0 for t ∈ λ, ∞. Proof. Let g1 t g t/t, g2 t t4−p g1 t and g3 t t4−p g2 5 t/4p2 p − 12 p 12 . Then simple computations lead to g1 0, 2.1 lim gt −∞, 2.2 t → ∞ g1 t − 2 p − 1 p 1 t2p 2p p 1 t2p−2 p p 1 p 3 2 × tp1 − 2 p 1 p 2 tp 2p p 1 p 3 tp−1 2.3 2 − 2p p 1 tp−2 p p 1 p − 1 tp−3 2 p 1 , g1 1 0, 2.4 lim g1 t −∞, 2.5 t → ∞ 2 g2 t − 4p p − 1 p 1 tp3 4p p 1 p − 1 tp1 p p 1 2 × p 3 t4 − 2p p 1 p 2 t3 2p p − 1 p 1 p 3 2.6 2 × t2 − 2p p 1 p − 2 t p p 1 p − 1 p − 3 , g2 1 0, 2.7 lim g2 t −∞, 2.8 t → ∞ 2 g2 t − 4p p − 1 p 1 p 3 tp2 4p p 1 p − 1 tp 2 2 4p p 1 p 3 t3 − 6p p 1 p 2 t2 2.9 2 4p p − 1 p 1 p 3 t − 2p p 1 p − 2 , g2 1 0, lim g t t → ∞ 2 −∞, 2.10 2.11 2 g2 t − 4p p − 1 p 1 p 2 p 3 tp1 4p2 p 1 2 2 × p − 1 tp−1 12p p 1 p 3 t2 − 12p p 1 × p 2 t 4p p − 1 p 1 p 3 , 2 g2 1 12p 2 − p p 1 > 0, lim g t t → ∞ 2 −∞, 2.12 2.13 2.14 4 Journal of Applied Mathematics 2 2 g2 t − 4p p − 1 p 1 p 2 p 3 tp 4p2 p 1 2 2 × p − 1 tp−2 24p p 1 p 3 t 2.15 2 − 12p p 1 p 2 , 2 g2 1 12p 2 − p 2p 3 p 1 > 0, lim g t t → ∞ 2 −∞, 2 2 4 g2 t − 4p2 p − 1 p 1 p 2 p 3 tp−1 4p2 p 1 2 2 × p − 1 p − 2 tp−3 24p p 1 p 3 , 2 4 g2 1 8p p 1 −4p3 2p2 5p 9 2 > 8p p 1 −4 × 1.83 2 × 1.752 5 × 1.75 9 2.16 2.17 2.18 2.19 2 4.376p p 1 > 0, 4 lim g t t → ∞ 2 −∞, g3 t − p 2 p 3 t2 p − 2 p − 3 ≤− p2 p3 p−2 p−3 2.20 2.21 −10p < 0 for t ∈ 1, ∞. 4 From the inequality 2.21 we clearly see that g2 t is strictly decreasing in 1, ∞. 4 Then 2.19 and 2.20 lead to the conclusion that there exists λ1 > 1 such that g2 t > 0 4 for t ∈ 1, λ1 and g2 t < 0 for t ∈ λ1 , ∞. Hence, g2 t is strictly increasing in 1, λ1 and strictly decreasing in λ1 , ∞. It follows from 2.16 and 2.17 together with the monotonicity of g2 t that there exists λ2 > 1 such that g2 t > 0 for t ∈ 1, λ2 and g2 t < 0 for t ∈ λ2 , ∞. Therefore, g2 t is strictly increasing in 1, λ2 and strictly decreasing in λ2 , ∞. From 2.13 and 2.14 together with the monotonicity of g2 t we know that there exists λ3 > 1 such that g2 t > 0 for t ∈ 1, λ3 and g2 t < 0 for t ∈ λ3 , ∞. So, g2 t is strictly increasing in 1, λ3 and strictly decreasing in λ3 , ∞. Equations 2.10 and 2.11 together with the monotonicity of g2 t imply that there exists λ4 > 1 such that g2 t > 0 for t ∈ 1, λ4 and g2 t < 0 for t ∈ λ4 , ∞. Hence, g2 t is strictly increasing in 1, λ4 and strictly decreasing in λ4 , ∞. It follows from 2.7 and 2.8 together with the monotonicity of g2 t that there exists λ5 > 1 such that g2 t > 0 for t ∈ 1, λ5 and g2 t < 0 for t ∈ λ5 , ∞. Therefore, g1 t is strictly increasing in 1, λ5 and strictly decreasing in λ5 , ∞. From 2.4 and 2.5 together with the monotonicity of g1 t we clearly see that there exists λ6 > 1 such that g1 t > 0 for t ∈ 1, λ6 and g1 t < 0 for t ∈ λ6 , ∞. So, gt is strictly increasing in 1, λ6 and strictly decreasing in λ6 , ∞. Journal of Applied Mathematics gt. 5 Therefore, Lemma 2.1 follows from 2.1 and 2.2 together with the monotonicity of 3. Main Result Theorem 3.1. The double inequality J2/π−2 a, b < T a, b < J2 a, b 3.1 holds for all a, b > 0 with a / b, and J2/π−2 a, b and J2 a, b are the best possible lower and upper one-parameter mean bounds for the Seiffert mean T a, b, respectively. Proof. Without loss of generality, we assume that a > b. Let t a/b > 1. Then from 1.1 and 1.2 we have b t2 t 1 t − 1 3 t2 − 1 4 arctan − . J2 a, b − T a, b 6t 1 arctant − 1/t 1 t 1 t2 t 1 3.2 Let t − 1 3 t2 − 1 ft 4 arctan − . t 1 t2 t 1 3.3 Then simple computations lead to f1 0, f t t − 14 t2 1t2 t 1 2 > 0, 3.4 for t > 1. Therefore, T a, b < J2 a, b for all a, b > 0 with a / b follows from 3.2–3.4. Next, we prove that T a, b > J2/π−2 a, b 3.5 for all a, b > 0 with a / b. Let p 2/π − 2 1.75 · · · . Then 1.1 and 1.2 lead to T a, b − Jp a, b bp tp1 − 1 2 p 1 tp − 1 arctant − 1/t 1 p 1 t − 1tp − 1 t−1 . − 2 arctan t1 p tp1 − 1 3.6 6 Journal of Applied Mathematics Let p 1 t − 1tp − 1 t−1 . − 2 arctan Gt t1 p tp1 − 1 3.7 Then simple computations lead to lim Gt lim Gt 0, 3.8 gt G t , 2 p1 p t − 1 t2 1 3.9 t→1 t → ∞ where gt is defined as in Lemma 2.1. From Lemma 2.1 and 3.9 we know that there exists λ > 1 such that Gt is strictly increasing in 1, λ and strictly decreasing in λ, ∞. Then 3.8 leads to that Gt > 0, 3.10 for t > 1. Therefore, the inequality 3.5 follows from 3.6, 3.7, and 3.10. Finally, we prove that J2/π−2 a, b and J2 a, b are the best possible lower and upper one-parameter mean bounds for the Seiffert mean T a, b, respectively. Let p 2/π − 2, 0 < ε < 2 and x > 0. Then from 1.1 and 1.2 one has Jpε x, 1 pε p π π × > × 1, x → ∞ T x, 1 pε1 2 p1 2 3.11 lim T 1 x, 1 − J2−ε 1 x, 1 hx , 2−ε 23 − ε 1 x − 1 arctanx/2 x 3.12 where hx 3 − εx 1 x2−ε − 1 − 22 − ε 1 x3−ε − 1 arctan x . 2x 3.13 Letting x → 0 and making use of Taylor expansion we get 2 − ε1 − ε 2 ε1 − ε2 − ε 3 x − x o x3 hx 3 − εx 2 − εx 2 6 3 − ε2 − ε 2 1 − ε2 − ε3 − ε 3 − 22 − ε 3 − εx x x o x3 2 6 x x2 x3 1 × − o x3 ε2 − ε3 − εx4 o x4 . 2 4 12 12 3.14 Journal of Applied Mathematics 7 The inequality 3.11 implies that for any 0 < ε < 2, there exists X Xε > 1, such that T x, 1 < J2/π−2ε x, 1 for x ∈ X, ∞. Equations 3.12–3.14 imply that for any 0 < ε < 2, there exists δ δε > 0 such that T 1 x, 1 > J2−ε 1 x, 1 for x ∈ 0, δ. 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