Sharp Inequalities Involving Neuman Means of the Second Kind with Applications
|
|
- Posy Nicholson
- 5 years ago
- Views:
Transcription
1 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly Sharp Ineqalities Involving Neman Means of the Second Kind with Applications Lin-Chang Shen, Ye-Ying Yang * Wei-Mao Qian 3 Hzho Shanlian Adlt School,Hzho, Zhejiang,China Mechanic Electronic Atomobile Egineering College, Hzho Vocational & Technical College, Hzho, Zhejiang,China 3 School of Distance Edcation, Hzho Broadcast TV University, Hzho, Zhejiang,China yyy008hz@63.com. Abstract In this paper, we give the eplicit formlas for Neman means of the second kind N GQ(a, b) N QG(a, b), find the best possible parameters α i, β i (0, )(i =,, 3,, 6) sch that the doble ineqalities α Q(a, b) + ( α )G(a, b) < N QG(a, b) < β Q(a, b) + ( β )G(a, b), α G(a, b) + α Q(a, b) < N QG(a, b) < β G(a, b) + β Q(a, b), α 3Q(a, b) + ( α 3)G(a, b) < N GQ(a, b) < β 3Q(a, b) + ( β 3)G(a, b), α 4 G(a, b) + α4 Q(a, b) < N GQ(a, b) < β4 G(a, b) + β4 Q(a, b), α 5Q(a, b) + ( α 5)V (a, b) < N QG(a, b) < β 5Q(a, b) + ( β 5)V (a, b), α 6Q(a, b) + ( α 6)U(a, b) < N GQ(a, b) < β 6Q(a, b) + ( β 6)U(a, b), holds for all a, b > 0 with a b, where G(a, b) Q(a, b) are the classical geometric qadratic means, V (a, b), U(a, b), N QG(a, b) N GQ(a, b) are Yang Neman mean of the second kind. Keywords: geometric mean, qadratic mean, Neman means of the second kind, Yang means, ineqalities. Introdction For a, b > 0 with a b, the Schwab-Borchardt mean SB(a, b), is defined by b a cos (a/b), if a < b, SB(a, b) = cosh (a/b), if a > b. where cos () cosh () = log( + ) are the inverse cosine inverse hyperbolic cosine fnctions, respectively. It is well-known that SB(a, b) is strictly increasing in both a b, nonsymmetric homogeneos of degree with respect to a b. Many symmetric bivariate means are special cases of the Schwab- Borchardt mean, for eample, the first second Seiffert means, Neman-Sándor mean, logarithmic mean two Yang means 3 are respectively defined by P = P (a, b) = sin = SB(G, A), ()/(a + b) T = T (a, b) = tan = SB(A, Q), ()/(a + b) Copyright 06 Isaac Scientific Pblishing
2 40 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly 06 M = M(a, b) = sinh = SB(Q, A), ()/(a + b) L = L(a, b) = tanh = SB(A, G), ()/(a + b) U = U(a, b) = tan ()/ = SB(G, Q), () ab V = V (a, b) = sinh ()/ = SB(Q, G). () ab where G = G(a, b) = ab, A = A(a, b) = (a + b)/ Q = Q(a, b) = (a + b )/ are the classical geometric, arithmetic qadratic means of a b. Let X = X(a, b) Y = Y (a, b) be the symmetric bivariate means of a b. Then Neman mean of the second kind N XY (a, b)4 is defined by N XY (a, b) = Y X +. (3) SB(X, Y ) Moreover, withot loss of generality, let a > b, v = ()/(a + b) (0, ), then Neman 4 gave eplicit formlas N AG (a, b) = A + ( v ) tanh (v) v N AQ (a, b) = A + ( + v ) tan (v) v ineqalities, N GA (a, b) = A v + sin (v) v, N QA (a, b) = A + v + sinh (v) v G(a, b) < L(a, b) < N AG (a, b) < P (a, b) < N GA (a, b) < A(a, b) < M(a, b) < N QA (a, b) < T (a, b) < N AQ (a, b) < Q(a, b). for all a, b > 0 with a b. In the recent past, the Schwab-Borchardt mean has been the sbject of intensive research. In particlar, many remarkable ineqalities for Schwab-Borchardt mean its generated means can be fond in the literatre 4-4. In 4, Neman fond the best possible constants α, α, α 3, α 4 β, β, β 3, β 4 sch that the doble ineqalities α A(a, b) + ( α )G(a, b) < N GA (a, b) < β A(a, b) + ( β )G(a, b) α Q(a, b) + ( α )A(a, b) < N AQ (a, b) < β Q(a, b) + ( β )A(a, b) α 3 A(a, b) + ( α 3 )G(a, b) < N AG (a, b) < β 3 A(a, b) + ( β 3 )G(a, b) α 4 Q(a, b) + ( α 4 )A(a, b) < N QA (a, b) < β 4 Q(a, b) + ( β 4 )A(a, b) hold for a, b > 0 with a b if only if α /3, β π/4, α /3, β (π )/ 4( ) = 0.689, α 3 /3, β 3 / α 4 /3, β 4 log( + ) + / ( ) = Zhang et al. presented the best possible parameters α, α, β, β 0, / α 3, α 4, β 3, β 4 /, sch that the doble ineqalities G ( α a + ( α )b, α b + ( α )a ) < N AG (a, b) < G ( β a + ( β )b, β b + ( β )a ) G ( α a + ( α )b, α b + ( α )a ) < N GA (a, b) < G ( β a + ( β )b, β b + ( β )a ) Q ( α 3 a + ( α 3 )b, α 3 b + ( α 3 )a ) < N QA (a, b) < Q ( β 3 a + ( β 3 )b, β 3 b + ( β 3 )a ) Q ( α 4 a + ( α 4 )b, α 4 b + ( α 4 )a ) < N AQ (a, b) < Q ( β 4 a + ( β 4 )b, β 4 b + ( β 4 )a ). Copyright 06 Isaac Scientific Pblishing
3 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly 06 4 hold for all a, b > 0 with a b. Go et.al. proved that the doble ineqalities A p (a, b)g p (a, b) < N GA (a, b) < A q (a, b)g q (a, b), p G(a, b) + p A(a, b) < N GA(a, b) < q G(a, b) + q A(a, b), A p3 (a, b)g p3 (a, b) < N AG (a, b) < A q3 (a, b)g q3 (a, b), p 4 G(a, b) + p 4 A(a, b) < N AG(a, b) < q 4 G(a, b) + q 4 A(a, b), Q p5 (a, b)a p5 (a, b) < N AQ (a, b) < Q q5 (a, b)a q5 (a, b), p 6 A(a, b) + p 6 Q(a, b) < N AQ(a, b) < q 6 A(a, b) + q 6 Q(a, b), Q p7 (a, b)a p7 (a, b) < N QA (a, b) < Q q7 (a, b)a q7 (a, b), p 8 A(a, b) + p 8 Q(a, b) < N QA(a, b) < q 8 A(a, b) + q 8 Q(a, b). hold for all a, b > 0 with a b if only if p /3, q, p 0, q /3, p 3 /3, q 3, p 4 0, q 4 /3, p 5 /3, q 5 log(π+)/ log 4 = 0.744, p 6 6+ (+ )π /(π+) = 0.49, q 6 /3, p 7 /3, q 7 log +log(+ ) / log = p 8 + (+ ) log(+ ) / + log( + ) = , q8 /3. Let a > b > 0, = ()/ ab (0, + ). Then from ()-(3) we gave the eplicit formlas N QG (a, b) = G(a, b) + + sinh (). (4) N GQ (a, b) = G(a, b) + ( + ) tan (). (5) The main prpose of this paper is to find the best possible parameters α i, β i (0, )(i =,, 3,, 6) sch that the doble ineqalities hold for all a, b > 0 with a b. α Q(a, b) + ( α )G(a, b) < N QG (a, b) < β Q(a, b) + ( β )G(a, b), α G(a, b) + α Q(a, b) < N QG (a, b) < β G(a, b) + β Q(a, b), α 3 Q(a, b) + ( α 3 )G(a, b) < N GQ (a, b) < β 3 Q(a, b) + ( β 3 )G(a, b), α 4 G(a, b) + α 4 Q(a, b) < N GQ (a, b) < β 4 G(a, b) + β 4 Q(a, b), α 5 Q(a, b) + ( α 5 )V (a, b) < N QG (a, b) < β 5 Q(a, b) + ( β 5 )V (a, b), α 6 Q(a, b) + ( α 6 )U(a, b) < N GQ (a, b) < β 6 Q(a, b) + ( β 6 )U(a, b). Lemma In order to prove or main reslts we need several lemmas, which we present in this section. Lemma. (see5) For < a < b < +, let f, g : a, b R be continos on a, b, be differentiable on (a, b), let g () 0 on (a, b). If f ()/g () is increasing (decreasing) on (a, b), then so are f() f(a) g() g(a), f() f(b) g() g(b) If f ()/g () is strictly monotone, then the monotonicity in the conclsion is also strict. Copyright 06 Isaac Scientific Pblishing
4 4 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly 06 Lemma. (see 6). Sppose that the power series f() = a n n g() = b n n have the radis of convergence r > 0 with a n, b n > 0 for all n = 0,,,. Let h() = f()/g(), if the seqence series {a n /b n } is (strictly) increasing (decreasing), then h() is also (strictly) increasing (decreasing) on (0, r). Lemma.3 () (See 7, Lemma.4) The fnction ϕ () = is strictly increasing from (0, + ) onto(/3, ). ()(See 7, Lemma.6) The fnction ϕ () = + sinh() 4 sinh() sinh() sinh() sinh() cosh() cosh() + sinh() cosh() is strictly decreasing from (0, + ) onto (0, /3). (3)(See 7, Lemma.5) The fnction ϕ 3 () = is strictly increasing from (0, π/) onto(8/3, π). (4)(See 7, Lemma.8) The fnction ϕ 4 () = sin() sin() cos() sin() cos() cos() + sin() cos() is strictly decreasing from (0, π/) onto(, /3). Lemma.4 The fnction ϕ 5 () = sinh() sinh() cosh() + is strictly decreasing from (0, + ) onto(, ). Proof. Let f () = sinh(), g () = sinh() cosh() +. Then simple comptations lead to ϕ 5 () = f () g () = f () f (0 + ) g () g (0 + ). (6) Let f () sinh() + cosh() 4 g = () cosh() sinh() n (n)! n + = n (n)! n = a n = n= n= (n+) n+ (n+)! n+ n+ (n+)! n+ 4 n n+ (n+)! n+ = (n + ) n+4 (n + 3)! > 0, b n = n+ (n+)! n+ (n+) n+4 (n+3)! n (n+) n+4 (n+3)! n. (n + ) n+4 (n + 3)! (7) > 0. (8) a n+ a n = b n+ b n (n + )(n + ) < 0. (9) Copyright 06 Isaac Scientific Pblishing
5 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly for all n 0. It follows from Lemma. (7)-(9) that f ()/g () is strictly decreasing on (0, + ). Note that ϕ 5 (0 + ) = a 0 b 0 =, ϕ 5 (+ ) =. (0) Therefore, Lemma.4 follows easily from Lemma. (6), (0) together with the monotonicity of f ()/g (). Lemma.5 The fnction ϕ 6 () = + sin() cos() sin () sin() sin() is strictly increasing from (0, π/) onto (0, (π 8)/(π )). Proof.The fnction ϕ 6 () can be rewritten as ϕ 6 () = + cos() sin() + = ϕ 7 () + ϕ 8 (). () sin() sin() where ϕ 7 () = / sin() ϕ 8 () = + cos() sin()/ sin(). Let f () = + cos() sin(), g () = sin(), f 3 () = cos() sin() g 3 () = cos(). Then simple comptations lead to ϕ 8 () = f () g () = f () f (0 + ) g () g (0 + ). () f () g () = f 3() g 3 () = f 3() f 3 (0 + ) g 3 () g 3 (0 + ). (3) f 3() g 3 () = tan(). (4) Since the fnction / tan() is strictly decreasing on (0, π/), hence Lemma. ()-(4) lead to that ϕ 8 () is strictly increasing on (0, π/). From () the fact that the fnction ϕ 7 () = / sin() is strictly increasing on (0, π/) together with the monotonicity of ϕ 8 () we can reach the conclsion that ϕ 6 () is strictly increasing on (0, π/). Note that ϕ 6 (0 + ) = 0, ϕ 6 ( π ) = π 8 (π ). (5) Therefore, Lemma.5 follows easily from (5) the monotonicity of ϕ 6 (). 3 Main Reslts Theorem 3. The doble ineqalities α Q(a, b) + ( α )G(a, b) < N QG (a, b) < β Q(a, b) + ( β )G(a, b). (6) α G(a, b) + α Q(a, b) < N QG (a, b) < β G(a, b) + β Q(a, b). (7) hold for all a, b > 0 with a b if only if α /3, β /, α 0 β /3. Proof.We clearly see that ineqalities (6) (7) can be rewritten as α < N QG(a, b) G(a, b) Q(a, b) G(a, b) < β. (8) α < /N QG(a, b) /Q(a, b) /G(a, b) /Q(a, b) < β. (9) Copyright 06 Isaac Scientific Pblishing
6 44 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly 06 respectively. Since both the geometric mean G(a, b) qadratic mean Q(a, b) are symmetric homogeneos of degree, withot loss of generality, we assme that a > b > 0. Let = ()/ ab (0, + ). Then from (4) (8)-(9) together with Q(a, b) = G(a, b) + we have α < + + sinh () + < β. (0) + α < sinh () ( + ) < β. () + + sinh () respectively. Let = sinh (). Then (0, + ), + + sinh () + = + sinh() 4 sinh() = sinh() sinh() ϕ (). () + sinh () ( + ) + + sinh () = sinh() cosh() cosh() + sinh() cosh() = ϕ (). where the fnctions ϕ () ϕ () are defined as in Lemma.3() (). Therefore, ineqality (6) holds for all a, b > 0 with a b if only if α /3 β / follows from (0) () together with Lemma.3(), ineqality (7) holds for all a, b > 0 with a b if only if α 0 β /3 follows from () (3) together with Lemma.3(). Theorem 3. The doble ineqalities α 3 Q(a, b) + ( α 3 )G(a, b) < N GQ (a, b) < β 3 Q(a, b) + ( β 3 )G(a, b). (4) (3) α 4 G(a, b) + α 4 Q(a, b) < N GQ (a, b) < β 4 G(a, b) + β 4 Q(a, b). (5) holds for all a, b > 0 with a b if only if α 3 /3, β 3 π/4, α 4 0 β 4 /3. Proof.We clearly see that ineqalities (4) (5) can be rewritten as α 3 < N GQ(a, b) G(a, b) Q(a, b) G(a, b) α 4 < /N GQ(a, b) /Q(a, b) /G(a, b) /Q(a, b) < β 3. (6) < β 4. (7) respectively. Since both the geometric mean G(a, b) qadratic mean Q(a, b) are symmetric homogeneos of degree, withot loss of generality, we assme that a > b > 0. Let = ()/ ab (0, + ). Then from (5) (6)-(7) together with Q(a, b) = G(a, b) + we have α 3 < + ( + ) tan () + < β 3. (8) Copyright 06 Isaac Scientific Pblishing
7 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly α 4 < + + ( + ) tan () ( < β 4. (9) + ) + ( + ) tan () respectively. Let = tan (). Then (0, π/), + ( + ) tan () + = sin() 4 sin() cos() = 4 ϕ 3(). + + ( + ) tan () ( + ) + ( + ) tan () = + sin() cos() cos() + sin() cos() = + ϕ 4(). (30) (3) where the fnctions ϕ 3 () ϕ 4 () are defined as in Lemma.3(3).3(4). Therefore, ineqality (4) holds for all a, b > 0 with a b if only if α 3 /3 β 3 π/4 follows from (8) (30) together with Lemma.3(3), ineqality (5) holds for all a, b > 0 with a b if only if α 4 0 β 4 /3 follows from (9) (3) together with Lemma.3(4). Theorem 3.3 The doble ineqalities α 5 Q(a, b) + ( α 5 )V (a, b) < N QG (a, b) < β 5 Q(a, b) + ( β 5 )V (a, b). (3) holds for all a, b > 0 with a b if only if α 5 0 β 5 /. Proof.We clearly see that ineqalities (3) can be rewritten as α 5 < N QG(a, b) V (a, b) Q(a, b) V (a, b) < β 5. (33) Since both the geometric mean G(a, b) qadratic mean Q(a, b) are symmetric homogeneos of degree, withot loss of generality, we assme that a > b > 0. Let = ()/ ab (0, + ). Then from (4) (33) together with Q(a, b) = G(a, b) + we have α 5 < + + sinh () + sinh () sinh () < β 5. (34) Let = sinh (). Then (0, + ), + + sinh () + sinh () sinh () = sinh() sinh() cosh() + = ϕ 5(). (35) where the fnctions ϕ 5 () is defined as in Lemma.4. Therefore, ineqality (3) holds for all a, b > 0 with a b if only if α 5 0 β 5 / follows from (34) (35) together with Lemma.4. Copyright 06 Isaac Scientific Pblishing
8 46 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly 06 Theorem 3.4 The doble ineqalities α 6 Q(a, b) + ( α 6 )U(a, b) < N GQ (a, b) < β 6 Q(a, b) + ( β 6 )U(a, b). (36) holds for all a, b > 0 with a b if only if α 6 0, β 6 (π 8)/4(π ) = Proof.We clearly see that ineqalities (36) can be rewritten as α 6 < N GQ(a, b) U(a, b) Q(a, b) U(a, b) < β 6. (37) Since both the geometric mean G(a, b) qadratic mean Q(a, b) are symmetric homogeneos of degree, withot loss of generality, we assme that a > b > 0. Let = ()/ ab (0, + ). Then from (5) (36) together with Q(a, b) = G(a, b) + we have α 6 < Let = tan (). Then (0, π/), + ( + ) tan () + + ( + ) tan () + tan () tan () tan () tan () < β 6. (38). = ϕ 6(), (39) where the fnction ϕ 6 () is defined as in Lemma.5. Therefore, ineqality (36) holds for all a, b > 0 with a b if only if α 6 0 β 6 (π 8)/4(π ) = follows from (37)-(39) together with Lemma.5. 4 Applications In this section, we will establish several sharp ineqalities involving the hyperbolic, inverse hyperbolic, trigonometric inverse trigonometric fnctions by se of Theorems From (3) we clearly see that N QG (a, b) = Q(a, b) + G (a, b) V (a, b), N GQ (a, b) = G(a, b) + Q (a, b) U(a, b) Let a > b = sinh ( a b ab ) (0, ). Then simple comptations lead to Q(a, b) V (a, b) = cosh(), G(a, b) G(a, b) = sinh() Theorems (40)-(4) lead to Theorem 4.. Theorem 4. The doble ineqalities α cosh() + ( α ) < cosh() +,. (40) U(a, b) G(a, b) = sinh() tan. (4) sinh() sinh() < β cosh() + ( β ), α cosh() + ( α ) < sinh() + < β cosh() + ( β ), α 3 cosh() + ( α 3 ) < cosh() coth() tan sinh() < β 3 cosh() + ( β 3 ), α 4 cosh() + ( α 4 ) cosh() < + cosh() coth() tan sinh() < β 4 cosh() + ( β 4 ), cosh() Copyright 06 Isaac Scientific Pblishing
9 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly α 5 cosh() + ( α 5 ) sinh() < cosh() + sinh() < β 5 cosh() + ( β 5 ) sinh(), sinh() α 6 cosh() + ( α 6 ) tan sinh() < + cosh() coth() tan sinh() sinh() < β 6 cosh() + ( β 6 ) tan sinh(). hold for all > 0 if only if α /3, β /, α 0, β /3, α 3 /3, β 3 π/4, α 4 0, β 4 /3, α 5 0, β 5 /, α 6 0 β 6 (π 8)/ 4(π ). Let a > b = tan ( ) a b ab (0, π/). Then it is not difficlt to verify that Q(a, b) V (a, b) = sec(), G(a, b) G(a, b) = From Theorems (40), (4) we get Theorem 4. immediately. Theorem 4. The doble ineqalities α sec() + ( α ) < sec() + sinh tan() tan() sinh U(a, b), tan() G(a, b) = tan(). (4) tan() < β sec() + ( β ), α + ( α ) cos() tan() < sec() tan() + sinh tan() < β + ( β ) cos(), α 3 sec() + ( α 3 ) < + sin() < β 3 sec() + ( β 3 ), α4 + ( α 4 ) cos() < sin() + < β4 + ( β 4 ) cos(), tan() α 5 sec()+( α 5 ) sinh tan() < sec()+ sinh tan() tan() < β 5 sec()+( β 5 ) tan() sinh tan(), α 6 sec() + ( α 6 ) tan() < + sin() < β 6 sec() + ( β 6 ) tan(). hold for all (0, π/) if only if α /3, β /, α 0, β /3, α 3 /3, β 3 π/4, α 4 0, β 4 /3, α 5 0, β 5 /, α 6 0 β 6 (π 8)/ 4(π ). Acknowledgments. This research was spported by the Natral Science Fondation of Zhejiang Broadcast TV University nder Grant XKT-5G7. References. E. Neman, J. Sándor, "On the Schwab-Borchardt mean", Math. Pann., vol.4, no., pp.53-66, E. Neman, J. Sándor, "On the Schwab-Borchardt mean II", Math. Pann., vol.7, no., pp.49-59, Z.-H.Yang, "Three families of two-parameter means constrcted by trigonometric fnctions", J. Ineqal. Appl., 54, 7 pages(03). 4. E. Neman, "On a new bivariate mean", Aeqat. Math., vol.88, no.3, pp.77-89, E. Neman, "On some means derived from the Schwab-Borchardt mean", J. Math. Ineqal., vol.8, pp., pp.7-83, E. Neman, "On some means derived from the Schwab-Borchardt mean II", J. Math. Ineqal.,vol.8, pp., , Y.-M. Ch, W.-M. Qian, L.-M. W, X.-H. Zhang, "Optimal bonds for the first second Seiffert means in terms of geometric, arithmetic contraharmonic means", J. Ineqal. Appl.,44(05). 8. Y.-M. Ch, W.-M. Qian, "Refinements of bonds for Neman means, Abstr". Appl. Anal., Article ID 543, 8 pages (004). Copyright 06 Isaac Scientific Pblishing
10 48 Jornal of Advances in Applied Mathematics, Vol., No. 3, Jly W.-M. Qian, Y.-M. Ch, "Optimal bonds for Neman means in terms of geometric, arithmetic qadratic means", J. Ineqal. Appl., 04:75 (04). 0. W.-M. Qian, Z.-H Shao Y.-M. Ch, "Sharp Ineqalities Involving Neman Means of the Second Kind", J. Math. Ineqal., vol.9, no. pp , 05.. Y. Zhang, Y.-M. Ch Y.-L. Jiang, "Sharp geometric mean bonds for Nemam means", Abstr. Appl. Anal., Article ID94988, 6 pages, (04).. Z.-J.Go, Y. zhang, Y.- M. Ch Y.-Q. Song, "Sharp bonds for Neman means in terms of geometric, arithmetic qadratic means", Available online at ariv. org/abs/ Y.-Y. Yang, W.-M. Qian, "The optimal conve combination bonds of harmonic, arithmetic contraharmonic means for the Neman means", Int. Math. Form, vol.9, no.7, pp , Z.-Y. He, Y.-M. Ch M.-K. Wang, "Optimal bonds for Neman means in terms of harmonic contraharmonic means", J. Appl. Math., Article ID 80763, 4 pages(03). 5. G. D. Anderson, M. K. Vamanamrthy M. K. Vorinen, Conformal Invariants, Ineqalities, Qasiconformal Maps, Canadian Mathematical Society Series of Monographs Advanced Tets, John Wiley & Sons, New York, NY, USA, S. Simić M. Vorinen, "Len ineqalities for zero-balanced hypergeometric fnction", Abstr. Appl. Anal., Article ID 9306, pages(0). 7. S.- B. Chen, Z.-Y. He, Y.-M. Ch, Y.-Q. Song X.-J. Tao, "Note on certain ineqalities for Neman means", J. Ineqal. Appl., 04:370(04). Copyright 06 Isaac Scientific Pblishing
ON YANG MEANS III. Edward Neuman
BULLETIN OF THE INTERNATIONAL MATHEMATICAL VIRTUAL INSTITUTE ISSN (p) 2303-4874, ISSN (o) 2303-4955 www.imvibl.org /JOURNALS / BULLETIN Vol. 8(2018), 113-122 DOI: 10.7251/BIMVI1801113N Former BULLETIN
More informationResearch Article On Certain Inequalities for Neuman-Sándor Mean
Abstract and Applied Analysis Volume 2013, Article ID 790783, 6 pages http://dxdoiorg/101155/2013/790783 Research Article On Certain Inequalities for Neuman-Sándor Mean Wei-Mao Qian 1 and Yu-Ming Chu 2
More informationBounds Improvement for Neuman-Sándor Mean Using Arithmetic, Quadratic and Contraharmonic Means 1
International Mathematical Forum, Vol. 8, 2013, no. 30, 1477-1485 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/imf.2013.36125 Bounds Improvement for Neuman-Sándor Mean Using Arithmetic, Quadratic
More informationarxiv: v1 [math.ca] 1 Nov 2012
A NOTE ON THE NEUMAN-SÁNDOR MEAN TIEHONG ZHAO, YUMING CHU, AND BAOYU LIU Abstract. In this article, we present the best possible upper and lower bounds for the Neuman-Sándor mean in terms of the geometric
More informationResearch Article Bounds for the Combinations of Neuman-Sándor, Arithmetic, and Second Seiffert Means in terms of Contraharmonic Mean
Abstract and Applied Analysis Volume 2013, Article ID 903982, 5 pages http://dx.doi.org/10.1155/2013/903982 Research Article Bounds for the Combinations of Neuman-Sándor, Arithmetic, and Second Seiffert
More informationSharp Bounds for Seiffert Mean in Terms of Arithmetic and Geometric Means 1
Int. Journal of Math. Analysis, Vol. 7, 01, no. 6, 1765-177 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/ijma.01.49 Sharp Bounds for Seiffert Mean in Terms of Arithmetic and Geometric Means 1
More informationOptimal bounds for Neuman-Sándor mean in terms of the convex combination of the logarithmic and the second Seiffert means
Chen et al. Journal of Inequalities and Applications (207) 207:25 DOI 0.86/s660-07-56-7 R E S E A R C H Open Access Optimal bounds for Neuman-Sándor mean in terms of the conve combination of the logarithmic
More informationOptimal bounds for the Neuman-Sándor mean in terms of the first Seiffert and quadratic means
Gong et al. Journal of Inequalities and Applications 01, 01:55 http://www.journalofinequalitiesandapplications.com/content/01/1/55 R E S E A R C H Open Access Optimal bounds for the Neuman-Sándor mean
More informationResearch Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls
Hindawi Pblishing Corporation Discrete Dynamics in Natre and Society Volme 2008 Article ID 149267 8 pages doi:101155/2008/149267 Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis
More informationResearch Article A Nice Separation of Some Seiffert-Type Means by Power Means
International Mathematics and Mathematical Sciences Volume 2012, Article ID 40692, 6 pages doi:10.1155/2012/40692 Research Article A Nice Separation of Some Seiffert-Type Means by Power Means Iulia Costin
More informationLazarević and Cusa type inequalities for hyperbolic functions with two parameters and their applications
Yang and Chu Journal of Inequalities and Applications 2015 2015:403 DOI 10.1186/s13660-015-0924-9 R E S E A R C H Open Access Lazarević and Cusa type inequalities for hyperbolic functions with two parameters
More informationOn Toader-Sándor Mean 1
International Mathematical Forum, Vol. 8, 213, no. 22, 157-167 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.12988/imf.213.3344 On Toader-Sándor Mean 1 Yingqing Song College of Mathematics and Computation
More informationCharacterizations of probability distributions via bivariate regression of record values
Metrika (2008) 68:51 64 DOI 10.1007/s00184-007-0142-7 Characterizations of probability distribtions via bivariate regression of record vales George P. Yanev M. Ahsanllah M. I. Beg Received: 4 October 2006
More informationOn the Iyengar Madhava Rao Nanjundiah inequality and its hyperbolic version
Notes on Number Theory and Discrete Mathematics Print ISSN 110 51, Online ISSN 67 875 Vol. 4, 018, No., 14 19 DOI: 10.7546/nntdm.018.4..14-19 On the Iyengar Madhava Rao Nanjundiah inequality and its hyperbolic
More informationOptimal Bounds for Neuman-Sándor Mean in Terms of the Convex Combination of Geometric and Quadratic Means
Mathematica Aeterna, Vol. 5, 015, no. 1, 83-94 Optimal Bounds for Neuman-Sándor Mean in Terms of the Convex Combination of Geometric Quadratic Means Liu Chunrong1 College of Mathematics Information Science,
More informationDOI: /j3.art Issues of Analysis. Vol. 2(20), No. 2, 2013
DOI: 10.15393/j3.art.2013.2385 Issues of Analysis. Vol. 2(20) No. 2 2013 B. A. Bhayo J. Sánor INEQUALITIES CONNECTING GENERALIZED TRIGONOMETRIC FUNCTIONS WITH THEIR INVERSES Abstract. Motivate by the recent
More informationON OPTIMALITY CONDITIONS FOR ABSTRACT CONVEX VECTOR OPTIMIZATION PROBLEMS
J. Korean Math. Soc. 44 2007), No. 4, pp. 971 985 ON OPTIMALITY CONDITIONS FOR ABSTRACT CONVEX VECTOR OPTIMIZATION PROBLEMS Ge Myng Lee and Kwang Baik Lee Reprinted from the Jornal of the Korean Mathematical
More informationSharp bounds for Seiffert and Neuman-Sándor means in terms of generalized logarithmic means
Chu et al. Journal of Inequalities and Applications 2013, 2013:10 R E S E A R C H Open Access Sharp bounds for Seiffert and Neuman-Sándor means in terms of generalized logarithmic means Yu-Ming Chu 1*,
More informationConditions for Approaching the Origin without Intersecting the x-axis in the Liénard Plane
Filomat 3:2 (27), 376 377 https://doi.org/.2298/fil7276a Pblished by Faclty of Sciences and Mathematics, University of Niš, Serbia Available at: http://www.pmf.ni.ac.rs/filomat Conditions for Approaching
More informationResearch Article On Jordan Type Inequalities for Hyperbolic Functions
Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 010, Article ID 6548, 14 pages doi:10.1155/010/6548 Research Article On Jordan Type Inequalities for Hyperbolic Functions
More informationNEW PERIODIC SOLITARY-WAVE SOLUTIONS TO THE (3+1)- DIMENSIONAL KADOMTSEV-PETVIASHVILI EQUATION
Mathematical and Comptational Applications Vol 5 No 5 pp 877-88 00 Association for Scientific Research NEW ERIODIC SOLITARY-WAVE SOLUTIONS TO THE (+- DIMENSIONAL KADOMTSEV-ETVIASHVILI EQUATION Zitian Li
More informationarxiv: v1 [math.ca] 19 Apr 2013
SOME SHARP WILKER TYPE INEQUALITIES AND THEIR APPLICATIONS arxiv:104.59v1 [math.ca] 19 Apr 01 ZHENG-HANG YANG Abstract. In this paper, we prove that for fied k 1, the Wilker type inequality ) sin kp +
More informationRestricted Three-Body Problem in Different Coordinate Systems
Applied Mathematics 3 949-953 http://dx.doi.org/.436/am..394 Pblished Online September (http://www.scirp.org/jornal/am) Restricted Three-Body Problem in Different Coordinate Systems II-In Sidereal Spherical
More informationBäcklund transformation, multiple wave solutions and lump solutions to a (3 + 1)-dimensional nonlinear evolution equation
Nonlinear Dyn 7 89:33 4 DOI.7/s7-7-38-3 ORIGINAL PAPER Bäcklnd transformation, mltiple wave soltions and lmp soltions to a 3 + -dimensional nonlinear evoltion eqation Li-Na Gao Yao-Yao Zi Y-Hang Yin Wen-Xi
More informationarxiv: v1 [math.ca] 4 Aug 2012
SHARP POWER MEANS BOUNDS FOR NEUMAN-SÁNDOR MEAN arxiv:08.0895v [math.ca] 4 Aug 0 ZHEN-HANG YANG Abstract. For a,b > 0 with a b, let N a,b) denote the Neuman-Sándor mean defined by N a,b) = arcsinh a+b
More informationMATH 1010E University Mathematics Lecture Notes (week 8) Martin Li
MATH 1010E University Mathematics Lecture Notes (week 8) Martin Li 1 L Hospital s Rule Another useful application of mean value theorems is L Hospital s Rule. It helps us to evaluate its of indeterminate
More informationSigmoid functions for the smooth approximation to x
Sigmoid functions for the smooth approimation to Yogesh J. Bagul,, Christophe Chesneau,, Department of Mathematics, K. K. M. College Manwath, Dist : Parbhani(M.S.) - 43505, India. Email : yjbagul@gmail.com
More informationSolutions to Math 152 Review Problems for Exam 1
Soltions to Math 5 Review Problems for Eam () If A() is the area of the rectangle formed when the solid is sliced at perpendiclar to the -ais, then A() = ( ), becase the height of the rectangle is and
More informationResearch Article Best Possible Bounds for Neuman-Sándor Mean by the Identric, Quadratic and Contraharmonic Means
Abstract and Applied Analysis Volume 01, Article ID 486, 1 pages http://dx.doi.org/10.1155/01/486 Research Article Best Possible Bounds for Neuman-Sándor Mean by the Identric, Quadratic and Contraharmonic
More informationAffine Invariant Total Variation Models
Affine Invariant Total Variation Models Helen Balinsky, Alexander Balinsky Media Technologies aboratory HP aboratories Bristol HP-7-94 Jne 6, 7* Total Variation, affine restoration, Sobolev ineqality,
More informationResearch Article Inequalities for Hyperbolic Functions and Their Applications
Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2010, Article ID 130821, 10 pages doi:10.1155/2010/130821 Research Article Inequalities for Hyperbolic Functions and Their
More informationResearch Article Sharp Bounds by the Generalized Logarithmic Mean for the Geometric Weighted Mean of the Geometric and Harmonic Means
Applied Mathematics Volume 2012, Article ID 480689, 8 pages doi:10.1155/2012/480689 Research Article Sharp Bounds by the Generalized Logarithmic Mean for the Geometric Weighted Mean of the Geometric and
More informationFUNCTIONS OF ONE VARIABLE FUNCTION DEFINITIONS
Page of 6 FUNCTIONS OF ONE VARIABLE FUNCTION DEFINITIONS 6. HYPERBOLIC FUNCTIONS These functions which are defined in terms of e will be seen later to be related to the trigonometic functions via comple
More informationRemarks on strongly convex stochastic processes
Aeqat. Math. 86 (01), 91 98 c The Athor(s) 01. This article is pblished with open access at Springerlink.com 0001-9054/1/010091-8 pblished online November 7, 01 DOI 10.1007/s00010-01-016-9 Aeqationes Mathematicae
More informationQUANTILE ESTIMATION IN SUCCESSIVE SAMPLING
Jornal of the Korean Statistical Society 2007, 36: 4, pp 543 556 QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Hosila P. Singh 1, Ritesh Tailor 2, Sarjinder Singh 3 and Jong-Min Kim 4 Abstract In sccessive
More informationApproximate Solution of Convection- Diffusion Equation by the Homotopy Perturbation Method
Gen. Math. Notes, Vol. 1, No., December 1, pp. 18-114 ISSN 19-7184; Copyright ICSRS Pblication, 1 www.i-csrs.org Available free online at http://www.geman.in Approximate Soltion of Convection- Diffsion
More information6.2. The Hyperbolic Functions. Introduction. Prerequisites. Learning Outcomes
The Hyperbolic Functions 6. Introduction The hyperbolic functions cosh x, sinh x, tanh x etc are certain combinations of the exponential functions e x and e x. The notation implies a close relationship
More informationLecture Notes for Math 1000
Lecture Notes for Math 1000 Dr. Xiang-Sheng Wang Memorial University of Newfoundland Office: HH-2016, Phone: 864-4321 Office hours: 13:00-15:00 Wednesday, 12:00-13:00 Friday Email: xswang@mun.ca Course
More informationPapers Published. Edward Neuman. Department of Mathematics, Southern Illinois University, Carbondale. and
Papers Published Edward Neuman Department of Mathematics, Southern Illinois University, Carbondale and Mathematical Research Institute, 144 Hawthorn Hollow, Carbondale, IL, 62903, USA 134. On Yang means
More informationInterval-Valued Fuzzy KUS-Ideals in KUS-Algebras
IOSR Jornal of Mathematics (IOSR-JM) e-issn: 78-578. Volme 5, Isse 4 (Jan. - Feb. 03), PP 6-66 Samy M. Mostafa, Mokhtar.bdel Naby, Fayza bdel Halim 3, reej T. Hameed 4 and Department of Mathematics, Faclty
More informationCRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE. Jingbo Xia
CRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE Jingbo Xia Abstract. Let H 2 (S) be the Hardy space on the nit sphere S in C n. We show that a set of inner fnctions Λ is sfficient for the prpose of determining
More informationAdmissibility under the LINEX loss function in non-regular case. Hidekazu Tanaka. Received November 5, 2009; revised September 2, 2010
Scientiae Mathematicae Japonicae Online, e-2012, 427 434 427 Admissibility nder the LINEX loss fnction in non-reglar case Hidekaz Tanaka Received November 5, 2009; revised September 2, 2010 Abstract. In
More informationA generalized Alon-Boppana bound and weak Ramanujan graphs
A generalized Alon-Boppana bond and weak Ramanjan graphs Fan Chng Department of Mathematics University of California, San Diego La Jolla, CA, U.S.A. fan@csd.ed Sbmitted: Feb 0, 206; Accepted: Jne 22, 206;
More informationLecture 3. Lecturer: Prof. Sergei Fedotov Calculus and Vectors. Exponential and logarithmic functions
Lecture 3 Lecturer: Prof. Sergei Fedotov 10131 - Calculus and Vectors Exponential and logarithmic functions Sergei Fedotov (University of Manchester) MATH10131 2011 1 / 7 Lecture 3 1 Inverse functions
More informationA New Proof of Inequalities for Gauss Compound Mean
Int. Journal of Math. Analysis, Vol. 4, 2010, no. 21, 1013-1018 A New Proof of Inequalities for Gauss Compound Mean Zhen-hang Yang Electric Grid Planning and Research Center Zhejiang Province Electric
More informationBLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students
BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they
More informationSolving the Lienard equation by differential transform method
ISSN 1 746-7233, England, U World Jornal of Modelling and Simlation Vol. 8 (2012) No. 2, pp. 142-146 Solving the Lienard eqation by differential transform method Mashallah Matinfar, Saber Rakhshan Bahar,
More informationElements of Coordinate System Transformations
B Elements of Coordinate System Transformations Coordinate system transformation is a powerfl tool for solving many geometrical and kinematic problems that pertain to the design of gear ctting tools and
More informationTHE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS
THE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS OMAR HIJAB Abstract. At the basis of mch of comptational chemistry is density fnctional theory, as initiated by the Hohenberg-Kohn theorem. The theorem
More informationSiberian Mathematical Journal, Vol. 45, No. 5, pp , 2004 Original Russian Text c 2004 Derevnin D. A., Mednykh A. D. and Pashkevich M. G.
Siberian Mathematical Jornal Vol. 45 No. 5 pp. 840-848 2004 Original Rssian Text c 2004 Derevnin D. A. Mednykh A. D. and Pashkevich M. G. On the volme of symmetric tetrahedron 1 D.A. Derevnin A.D. Mednykh
More informationA Model-Free Adaptive Control of Pulsed GTAW
A Model-Free Adaptive Control of Plsed GTAW F.L. Lv 1, S.B. Chen 1, and S.W. Dai 1 Institte of Welding Technology, Shanghai Jiao Tong University, Shanghai 00030, P.R. China Department of Atomatic Control,
More informationB-469 Simplified Copositive and Lagrangian Relaxations for Linearly Constrained Quadratic Optimization Problems in Continuous and Binary Variables
B-469 Simplified Copositive and Lagrangian Relaxations for Linearly Constrained Qadratic Optimization Problems in Continos and Binary Variables Naohiko Arima, Snyong Kim and Masakaz Kojima October 2012,
More informationOn Multiobjective Duality For Variational Problems
The Open Operational Research Jornal, 202, 6, -8 On Mltiobjective Dality For Variational Problems. Hsain *,, Bilal Ahmad 2 and Z. Jabeen 3 Open Access Department of Mathematics, Jaypee University of Engineering
More informationMath 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation:
Math 263 Assignment #3 Soltions 1. A fnction z f(x, ) is called harmonic if it satisfies Laplace s eqation: 2 + 2 z 2 0 Determine whether or not the following are harmonic. (a) z x 2 + 2. We se the one-variable
More informationSUBORDINATION RESULTS FOR A CERTAIN SUBCLASS OF NON-BAZILEVIC ANALYTIC FUNCTIONS DEFINED BY LINEAR OPERATOR
italian jornal of pre and applied mathematics n. 34 215 375 388) 375 SUBORDINATION RESULTS FOR A CERTAIN SUBCLASS OF NON-BAZILEVIC ANALYTIC FUNCTIONS DEFINED BY LINEAR OPERATOR Adnan G. Alamosh Maslina
More informationcos t 2 sin 2t (vi) y = cosh t sinh t (vii) y sin x 2 = x sin y 2 (viii) xy = cot(xy) (ix) 1 + x = sin(xy 2 ) (v) g(t) =
MATH1003 REVISION 1. Differentiate the following functions, simplifying your answers when appropriate: (i) f(x) = (x 3 2) tan x (ii) y = (3x 5 1) 6 (iii) y 2 = x 2 3 (iv) y = ln(ln(7 + x)) e 5x3 (v) g(t)
More informationMAXIMUM AND ANTI-MAXIMUM PRINCIPLES FOR THE P-LAPLACIAN WITH A NONLINEAR BOUNDARY CONDITION. 1. Introduction. ν = λ u p 2 u.
2005-Ojda International Conference on Nonlinear Analysis. Electronic Jornal of Differential Eqations, Conference 14, 2006, pp. 95 107. ISSN: 1072-6691. URL: http://ejde.math.txstate.ed or http://ejde.math.nt.ed
More informationA new integral transform on time scales and its applications
Agwa et al. Advances in Difference Eqations 202, 202:60 http://www.advancesindifferenceeqations.com/content/202//60 RESEARCH Open Access A new integral transform on time scales and its applications Hassan
More informationMixed Type Second-order Duality for a Nondifferentiable Continuous Programming Problem
heoretical Mathematics & Applications, vol.3, no.1, 13, 13-144 SSN: 179-9687 (print), 179-979 (online) Scienpress Ltd, 13 Mied ype Second-order Dality for a Nondifferentiable Continos Programming Problem.
More information10.7. DIFFERENTIATION 7 (Inverse hyperbolic functions) A.J.Hobson
JUST THE MATHS SLIDES NUMBER 0.7 DIFFERENTIATION 7 (Inverse hyperbolic functions) by A.J.Hobson 0.7. Summary of results 0.7.2 The erivative of an inverse hyperbolic sine 0.7.3 The erivative of an inverse
More information4. Functions of one variable
4. Functions of one variable These lecture notes present my interpretation of Ruth Lawrence s lecture notes (in Hebrew) 1 In this chapter we are going to meet one of the most important concepts in mathematics:
More informationThe Scalar Conservation Law
The Scalar Conservation Law t + f() = 0 = conserved qantity, f() =fl d dt Z b a (t, ) d = Z b a t (t, ) d = Z b a f (t, ) d = f (t, a) f (t, b) = [inflow at a] [otflow at b] f((a)) f((b)) a b Alberto Bressan
More informationResearch Article On New Wilker-Type Inequalities
International Scholarly Research Network ISRN Mathematical Analysis Volume 2011, Article ID 681702, 7 pages doi:10.5402/2011/681702 Research Article On New Wilker-Type Inequalities Zhengjie Sun and Ling
More informationm = Average Rate of Change (Secant Slope) Example:
Average Rate o Change Secant Slope Deinition: The average change secant slope o a nction over a particlar interval [a, b] or [a, ]. Eample: What is the average rate o change o the nction over the interval
More information90 Chapter 5 Logarithmic, Exponential, and Other Transcendental Functions. Name Class. (a) (b) ln x (c) (a) (b) (c) 1 x. y e (a) 0 (b) y.
90 Chapter 5 Logarithmic, Eponential, and Other Transcendental Functions Test Form A Chapter 5 Name Class Date Section. Find the derivative: f ln. 6. Differentiate: y. ln y y y y. Find dy d if ey y. y
More informationSubcritical bifurcation to innitely many rotating waves. Arnd Scheel. Freie Universitat Berlin. Arnimallee Berlin, Germany
Sbcritical bifrcation to innitely many rotating waves Arnd Scheel Institt fr Mathematik I Freie Universitat Berlin Arnimallee 2-6 14195 Berlin, Germany 1 Abstract We consider the eqation 00 + 1 r 0 k2
More informationChapter 5 Logarithmic, Exponential, and Other Transcendental Functions
Chapter 5 Logarithmic, Exponential, an Other Transcenental Functions 5.1 The Natural Logarithmic Function: Differentiation 5.2 The Natural Logarithmic Function: Integration 5.3 Inverse Functions 5.4 Exponential
More informationVectors in Rn un. This definition of norm is an extension of the Pythagorean Theorem. Consider the vector u = (5, 8) in R 2
MATH 307 Vectors in Rn Dr. Neal, WKU Matrices of dimension 1 n can be thoght of as coordinates, or ectors, in n- dimensional space R n. We can perform special calclations on these ectors. In particlar,
More informationWe automate the bivariate change-of-variables technique for bivariate continuous random variables with
INFORMS Jornal on Compting Vol. 4, No., Winter 0, pp. 9 ISSN 09-9856 (print) ISSN 56-558 (online) http://dx.doi.org/0.87/ijoc.046 0 INFORMS Atomating Biariate Transformations Jeff X. Yang, John H. Drew,
More informationOPTIMAL INEQUALITIES BETWEEN GENERALIZED LOGARITHMIC, IDENTRIC AND POWER MEANS
International Journal of Pure and Applied Mathematics Volume 80 No. 1 01, 41-51 ISSN: 1311-8080 (printed version) url: http://www.ijpam.eu PA ijpam.eu OPTIMAL INEQUALITIES BETWEEN GENERALIZED LOGARITHMIC,
More informationThe Replenishment Policy for an Inventory System with a Fixed Ordering Cost and a Proportional Penalty Cost under Poisson Arrival Demands
Scientiae Mathematicae Japonicae Online, e-211, 161 167 161 The Replenishment Policy for an Inventory System with a Fixed Ordering Cost and a Proportional Penalty Cost nder Poisson Arrival Demands Hitoshi
More informationDifferential and Integral Calculus
School of science an engineering El Akhawayn University Monay, March 31 st, 2008 Outline 1 Definition of hyperbolic functions: The hyperbolic cosine an the hyperbolic sine of the real number x are enote
More informationXihe Li, Ligong Wang and Shangyuan Zhang
Indian J. Pre Appl. Math., 49(1): 113-127, March 2018 c Indian National Science Academy DOI: 10.1007/s13226-018-0257-8 THE SIGNLESS LAPLACIAN SPECTRAL RADIUS OF SOME STRONGLY CONNECTED DIGRAPHS 1 Xihe
More informationYong Luo, Shun Maeta Biharmonic hypersurfaces in a sphere Proceedings of the American Mathematical Society DOI: /proc/13320
Yong Lo, Shn aeta Biharmonic hypersrfaces in a sphere Proceedings of the American athematical Society DOI: 10.1090/proc/13320 Accepted anscript This is a preliminary PDF of the athor-prodced manscript
More informationMonotonicity rule for the quotient of two functions and its application
Yang et al. Journal of Inequalities and Applications 017 017:106 DOI 10.1186/s13660-017-1383- RESEARCH Open Access Monotonicity rule for the quotient of two functions and its application Zhen-Hang Yang1,
More informationTest one Review Cal 2
Name: Class: Date: ID: A Test one Review Cal 2 Short Answer. Write the following expression as a logarithm of a single quantity. lnx 2ln x 2 ˆ 6 2. Write the following expression as a logarithm of a single
More information4.2 First-Order Logic
64 First-Order Logic and Type Theory The problem can be seen in the two qestionable rles In the existential introdction, the term a has not yet been introdced into the derivation and its se can therefore
More informationCHAPTER 4. Elementary Functions. Dr. Pulak Sahoo
CHAPTER 4 Elementary Functions BY Dr. Pulak Sahoo Assistant Professor Department of Mathematics University Of Kalyani West Bengal, India E-mail : sahoopulak1@gmail.com 1 Module-4: Multivalued Functions-II
More informationNonlocal Symmetries and Interaction Solutions for Potential Kadomtsev Petviashvili Equation
Commn. Theor. Phs. 65 (16) 31 36 Vol. 65, No. 3, March 1, 16 Nonlocal Smmetries and Interaction Soltions for Potential Kadomtsev Petviashvili Eqation Bo Ren ( ), Jn Y ( ), and Xi-Zhong Li ( ) Institte
More informationBounded perturbation resilience of the viscosity algorithm
Dong et al. Jornal of Ineqalities and Applications 2016) 2016:299 DOI 10.1186/s13660-016-1242-6 R E S E A R C H Open Access Bonded pertrbation resilience of the viscosity algorithm Qiao-Li Dong *, Jing
More informationUttam Ghosh (1), Srijan Sengupta (2a), Susmita Sarkar (2b), Shantanu Das (3)
Analytical soltion with tanh-method and fractional sb-eqation method for non-linear partial differential eqations and corresponding fractional differential eqation composed with Jmarie fractional derivative
More informationENGI 3425 Review of Calculus Page then
ENGI 345 Review of Calculus Page 1.01 1. Review of Calculus We begin this course with a refresher on ifferentiation an integration from MATH 1000 an MATH 1001. 1.1 Reminer of some Derivatives (review from
More informationRight Trapezoid Cover for Triangles of Perimeter Two
Kasetsart J (Nat Sci) 45 : 75-7 (0) Right Trapezoid Cover for Triangles of Perimeter Two Banyat Sroysang ABSTRACT A convex region covers a family of arcs if it contains a congrent copy of every arc in
More informationOn Generalizations of Asymptotically AdS 3 Spaces and Geometry of SL(N)
EJTP 9, No. 7 01) 49 56 Electronic Jornal of Theoretical Physics On Generalizations of Asymptotically AdS 3 Spaces and Geometry of SLN) Heikki Arponen Espoontie 1 A, 0770 Espoo, Finland Received 30 October
More informationEOQ Problem Well-Posedness: an Alternative Approach Establishing Sufficient Conditions
pplied Mathematical Sciences, Vol. 4, 2, no. 25, 23-29 EOQ Problem Well-Posedness: an lternative pproach Establishing Sfficient Conditions Giovanni Mingari Scarpello via Negroli, 6, 226 Milano Italy Daniele
More informationFlexure of Thick Simply Supported Beam Using Trigonometric Shear Deformation Theory
International Jornal of Scientific and Research Pblications, Volme, Isse 11, November 1 1 ISSN 5-15 Flere of Thick Simply Spported Beam Using Trigonometric Shear Deformation Theory Ajay G. Dahake *, Dr.
More informationMath 180 Prof. Beydler Homework for Packet #5 Page 1 of 11
Math 180 Prof. Beydler Homework for Packet #5 Page 1 of 11 Due date: Name: Note: Write your answers using positive exponents. Radicals are nice, but not required. ex: Write 1 x 2 not x 2. ex: x is nicer
More information7.1. Calculus of inverse functions. Text Section 7.1 Exercise:
Contents 7. Inverse functions 1 7.1. Calculus of inverse functions 2 7.2. Derivatives of exponential function 4 7.3. Logarithmic function 6 7.4. Derivatives of logarithmic functions 7 7.5. Exponential
More informationA Contraction of the Lucas Polygon
Western Washington University Western CEDAR Mathematics College of Science and Engineering 4 A Contraction of the Lcas Polygon Branko Ćrgs Western Washington University, brankocrgs@wwed Follow this and
More informationA GEOMETRIC PROPERTY OF THE ROOTS OF CHEBYSHEV POLYNOMIALS
Journal of Applied Mathematics and Computational Mechanics 014, 13(1), 143-148 A GEOMETRIC PROPERTY OF THE ROOTS OF CHEBYSHEV POLYNOMIALS Roman Wituła, Edyta Hetmaniok, Damian Słota Institute of Mathematics,
More informationCHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES. George P. Yanev
Pliska Std. Math. Blgar. 2 (211), 233 242 STUDIA MATHEMATICA BULGARICA CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES George P. Yanev We prove that the exponential
More informationAsymptotics of dissipative nonlinear evolution equations with ellipticity: different end states
J. Math. Anal. Appl. 33 5) 5 35 www.elsevier.com/locate/jmaa Asymptotics of dissipative nonlinear evoltion eqations with ellipticity: different end states enjn Dan, Changjiang Zh Laboratory of Nonlinear
More informationUNIT NUMBER DIFFERENTIATION 7 (Inverse hyperbolic functions) A.J.Hobson
JUST THE MATHS UNIT NUMBER 0.7 DIFFERENTIATION 7 (Inverse hyperbolic functions) by A.J.Hobson 0.7. Summary of results 0.7.2 The erivative of an inverse hyperbolic sine 0.7.3 The erivative of an inverse
More informationTravelling Wave Solutions for the Gilson-Pickering Equation by Using the Simplified G /G-expansion Method
ISSN 1749-3889 (print, 1749-3897 (online International Journal of Nonlinear Science Vol8(009 No3,pp368-373 Travelling Wave Solutions for the ilson-pickering Equation by Using the Simplified /-expansion
More informationChapter 3 Differentiation Rules (continued)
Chapter 3 Differentiation Rules (continued) Sec 3.5: Implicit Differentiation (continued) Implicit Differentiation What if you want to find the slope of the tangent line to a curve that is not the graph
More informationRobust Tracking and Regulation Control of Uncertain Piecewise Linear Hybrid Systems
ISIS Tech. Rept. - 2003-005 Robst Tracking and Reglation Control of Uncertain Piecewise Linear Hybrid Systems Hai Lin Panos J. Antsaklis Department of Electrical Engineering, University of Notre Dame,
More informationThe Brauer Manin obstruction
The Braer Manin obstrction Martin Bright 17 April 2008 1 Definitions Let X be a smooth, geometrically irredcible ariety oer a field k. Recall that the defining property of an Azmaya algebra A is that,
More informationcosh x sinh x So writing t = tan(x/2) we have 6.4 Integration using tan(x/2) 2t 1 + t 2 cos x = 1 t2 sin x =
6.4 Integration using tan/ We will revisit the ouble angle ientities: sin = sin/ cos/ = tan/ sec / = tan/ + tan / cos = cos / sin / tan = = tan / sec / tan/ tan /. = tan / + tan / So writing t = tan/ we
More informationarxiv: v5 [math.ca] 28 Apr 2010
On Jordan type inequalities for hyperbolic functions R. Klén, M. Visuri and M. Vuorinen Department of Mathematics, University of Turku, FI-004, Finland arxiv:0808.49v5 [math.ca] 8 Apr 00 Abstract. This
More information