Modified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations

Size: px
Start display at page:

Download "Modified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations"

Transcription

1 Noliear Aalysis ad Differetial Equatios, Vol. 5, 27, o. 4, 57-7 HIKARI Ltd, Modified Decompositio Method by Adomia ad Rach for Solvig Noliear Volterra Itegro- Differetial Equatios M. Al-Mazmumy Departmet of Mathematics, Faculty of Sciece-AL Faisaliah Campus Kig Abdulaziz Uiversity, Jeddah, Saudi Arabia S. O. Almuhalbedi Departmet of Mathematics; Faculty of Sciece Kig Abdulaziz Uiversity Jeddah, Saudi Arabia Copyright 27 M. Al-Mazmumy ad S. O. Almuhalbedi. This article is distributed uder the Creative Commos Attributio Licese, which permits urestricted use, distributio, ad reproductio i ay medium, provided the origial work is properly cited. Abstract I this paper, Modified Decompositio Method by Adomia ad Rach has bee implemeted to aalyze oliear Volterra itegro-differetial equatios. The suggested approach is much better tha the stadard versio of the Adomia decompositio method. Some examples are provided to illustrate the method. Mathematics Subject Classificatio: 45D5; 45E; 65M2 Keywords: Adomia decompositio method; Modified Decompositio Method by Adomia ad Rach; Volterra itegro-differetial equatios; oliear itegrodifferetial equatios. Itroductio I 99, Adomia ad Rach [] itroduced a modificatio to the classical Adomia method, based o Multiple decompositio. For computatioal coveiece purpose, they itroduced the decompositio of both the system iputs ad system operators together with the solutio process to achieve simple to itegrate series for liear ad oliear differetial equatios. I 99, Adomia ad Rach [2] defied a oliear Trasformatio Series that will be

2 58 M. Al-Mazmumy ad S. O. Almuhalbedi evaluated usig the Adomia polyomials i the decompositio method. Give a specific fuctio N(u(t)) with u give by a coverget series, the evaluatio of N(u(t)) ca be made by usig the Adomia polyomials used to represet the oliearities i differetial ad partial differetial equatios. For a aalytic fuctio N(u(t)),, it ca be writte N(u(t)) = = A ( u, u u 2,, u ) where the A, are give by A = = c(ν, ) N (ν) (u) u=u,. To determie c(ν, ), the sum of possible products of v compoets u i ca be formed, with i =,, 2,..., ad divide by the factorial of the umber of repetitios of the compoets. I [2] Adomia ad Rach proposed the coverget series N(u) with u = c x, ad they stated the followig theorem: = Theorem : N(u) = N( = c x ) = = A ( c, c c 2,, c ). I 992, Adomia ad Rach [3] geeralized the theorem o trasformatio of series preseted i Ref.[2] to fuctio of several variables. The result is valuable i derivig solutios of coupled ordiary differetial equatios with geeral oliear couplig terms. Usig the modified decompositio method of the authors, they stated the followig theorems: Theorem 2. If u = = a x, ad v = = b x, the N(u, v) = N( = A x ), A = A ( a, a,, a, b, b, b ) where the A are Adomia polyomials of fuctios of two variables N(u, v). This ca be exteded to -dimesios ad -dimesioal Adomia polyomials. I iitial-value problem defied by a system of liear homogeeous differetial equatios, the power series solutios yields simple recurrece relatios for the coefficiets. But such solutios are geerally ot adequate for oliear equatios, although they are applicable to some simple cases such as the Riccati equatio. The results from the Adomia decompositio method [] ad Theorem 2 were used by Adomia ad Rach o trasformatio of series, stated i Theorem, i order to exted the Maclauri method. Adomia solved the geeral operator equatios Fu = g by usig the decompositio u = = u, which is a special case of the expasio of N(u) = = A ( u, u u 2,, u ). The coefficiets A are derived by coveiet algorithms for N(u). Thus, N( = u ) = = A ( u, u u 2,, u ). If u is give by the series u = = c x, each compoet u of the power series ca be idetified. This will lead to A ( u,, u ) = x A ( c,, c ). The series = x A ( c,, c ) is coverget if the series = c x is coverget. This is simply a extesio to Taylor series: N ( c (x x ) ) = A ( c, c,, c )(x x ) = =

3 Modified decompositio method by Adomia ad Rach 59 Thus, the Adomia series is actually a geeralized form of Taylor series about a fuctio rather tha a poit. I a liear case, it ca be reduced to the well-kow Taylor series. Further, Maclauri series ca be made more useful by combiig it with Adomia polyomials ad decompositio techiques. I Refereces [2] ad [3], the authors showed that the exteded Maclauri series ca be used for coupled differetial equatios ad partial differetial equatios. They also showed that the Adomia series resultig from the decompositio method has superior covergece properties, i spite the improved power of the Maclauri series with the use of the Adomia polyomials ad decompositio techiques. It is also evidet that the power series solutio becomes complicated i collectig terms, while the decompositio series is always simple i this respect. Further work to Adomia ad Rach [4] showed the applicability of the method for the solutio of liear or oliear partial differetial equatios ad coupled equatios; ad they also showed that the covergece is faster usig Adomia decompositio series tha usig the exteded or improved power series. Usig the cocept of modified decompositio series, Adomia ad Rach [5] established that ihomogeeous oliear partial differetial equatios with variable coefficiets ad iputs are solvable ad the coefficiets were easily programmable. Also, they foud the solutios of oliear partial differetial equatios usig a exteded Maclauri series form of the decompositio method ad the Adomia polyomials [6]. Recetly, several other researchers have applied this modificatio for solvig a wide class of problems. Lazhar Bougoffa [7] studied the solvability of the predator ad prey system with variable coefficiets ad showed the compariso of the results with this modified decompositio method. I Ref. [8], M. Almazmumy, et al. used this modificatio i the solutio of the iitial value problems i ordiary differetial equatios. 2. Modified Decompositio Method by Adomia ad Rach We cosider the itegro-differetial equatio of the form u (x) = f(x) + b(x) a k(x, t). (Lu(t) + N(u(t))dt (2.) with iitial coditios u() = α, u () = β. x x Let L = d2 dx 2, so L (. ) = (. )dxdx, applyig L to both sides of (2.), ad usig iitial coditios, we obtai: u(x) = α + βx + L f(x) + L b(x) a k(x, t). (Lu(t) + Nu(t)) dt (2.2) We proceed the solutio u(x), the ihomogeeous term ad the oliear term i a series form u(x) = = a x (2.3) f(x) = = b x (2.4)

4 6 M. Al-Mazmumy ad S. O. Almuhalbedi N(u) = = A x (2.5) where the polyomials A, =,, are called Adomia polyomials, ad let the kerel be formed as k(x, t) = m= = c m, x m t = = c (x)t (2.6) where c (x) = m= c m, x m. Substitutig (2.3)- (2.6) i (2.2) gives = a x = α + βx + L = b x + +L b(x) c m, x m t ( = a t + = A t )dt (2.7) a = m= Thus = a x = α + βx + L = b x + +L b(x) [ c m, x m t ( = t (a + A ))] dt (2.8) a = m= We observe that ( = c m, t )( = a t ) = = t ( c m,v (a v ) ad Substitutig v= ) v= ) ( = c m, t )( = A t ) = = t ( c m,v (A v ) = a x = α + βx + L = b x + L b(x) [ x m t. (a v + A v )]dt a = m= v= c m,v So that = a x = α + βx + L b x + L [ = m= v= c m,v (a v + A v )dt = x m++ + = a x b = α + βx + = (+)(+2) x+2 + m= x +m+3 = c (+)(m++2)(m++3) v= m,v (a v + A v ) The = a x = α + βx + b 2 =2 ( ) x + m= x m+ 3 =3 c ( 2)(m+ )(m+) v= m,v (a v 3 + A v 3 ) So that a + a x + a 2 x 2 + =3 =3 a x = α + βx + 2 b x 2 + x m+ =3 ( ) b 2x + m= v= c m,v. (a v 3 + A v 3 ) ( 2)(m+ )(m+) 3

5 Modified decompositio method by Adomia ad Rach 6 Equatig the coefficiets of like powers of x i both sides a = α a = β a 2 = 2 b a = b ( ) c ( 2)( ) v=,v. (a v 3 + A v 3 ) a +m =, m (2.9) By determie the coefficiet ad substitutig i (2.3) we get the solutio. 3. Computatioal results Example 2. Cosider oliear Volterra itegro-differetial equatio u (x) = e x + 2 e2x x 2 u2 (t)dt, u() = With the exact solutio is u(x) = e x. Applyig L x (. ) = (. )dx i both sides give u(x) = L (e x + 2 e2x x 2 ) L u 2 (t)dt Busig modified decompositio method by Adomia ad Rach (MDAR), leadig to x A 2 =2 ( ) x = a x = + L b x L = A t dt = the a x = + a + a x + Where, =2 b x = = = b x a x = + b x + = L (e x + 2 e2x ) 2 Equatig the coefficiets =2 b x A 2 =2 ( ) x = e x + 4 e2x x = x + x2 + 2 x3 +

6 62 M. Al-Mazmumy ad S. O. Almuhalbedi b = b = 2 b 2 = 3 2 b 3 = We ow get the recursive relatio a = a = a = b A 2 ( ), 2 or a = a = a 2 = b 2 A 2 = 2 a 3 = b 2 3 A 6 = 3! a 4 = b 3 4 A 2 2 = 4! The exact solutio is give by u(x) = = a x = + x + 2 x2 + 3! x3 + 4! x4 + = e x Example 2.2 Cosider the system of oliear Volterra itegro-differetial equatio u x (x) = 2 3x 2 si(x) + 3 cos(x) + (u 2 (t) + v 2 (t))dt, u() = v (t) = 2 + si(x) + 2 cos(x) + si(2x) + 2 x (u2 (t) v 2 (t))dt, v() = 2 With the exact solutio (u(x), v(x)) = ( + si(x), + cos(x)). ApplyigL x (. ) = (. )dx i both sides u(x) = 2x 3 x 2 x2 + 2 cos(x) si(x) + L (u 2 (t) + v 2 (t))dt, v(x) = 2 + 2x cos(x) + 2 si(x) 4 cos(2x) + 5 x 4 + L (u 2 (t) v 2 (t))dt Usig the method (MDAR) we get

7 Modified decompositio method by Adomia ad Rach 63 = a x = + L b x + L ( A t + = = = B t )dt g x = 2 + L R x + L x = = ( A t = = B t )dt So that a + a x + g + g x + Where = Ad b x R = =2 =2 a x = + b x + g x = 2 + R x + x b =2 R =2 = ( 2x 3 2 x2 + 2 cos(x) 2 + 3si (x)) = x 5 2 x2 2 x3 + 2 x4 + 4 x5 + x = ( 2x cos(x) + 2 si(x) cos(2x) + 5 ) 4 4 =x 2 3 x x4 + 6 x5 + Equatig coefficiets ( ) x x + =2 (A 2 _ + B 2 ) ( ) x x + =2 (A 2 B 2 ) b = b = 5 b 2 = 3 2 b 3 = 3, R = R = 2 R 2 = R 3 = 5 6 b 4 = 8. R 4 = 2 We ow get the recursive relatio a = a = b a = b + ( ) (A 2 + B 2 ), 2 ad g = g = R g = R + ( ) (A 2 B 2 ), 2 or

8 64 M. Al-Mazmumy ad S. O. Almuhalbedi a = a = b = a 2 = 2 b + 2 (A + b ) = a 3 = 3 b (A + b ) = 6 a 4 = 4 b (A 2 + b 2 ) = a 5 = b (A b 3 ) = 2 ad g = 2 g = R = g 2 = 2 R + 2 (A b ) = 2 g 3 = 3 R (A b ) = g 4 = 4 R (A 2 b 2 ) = 24 g 5 = 5 R (A 3 b 3 ) = The the series solutio ca be writte as u(x) = = a x = a + a x + a 2 x = + x 3! x3 + 5! x v(x) = = g x = g + g x + gx 2 + = + ( 2! x2 + 4! x4 +.. ) Or u(x) = + si(x) v(x) = + cos(x) Example 2.3 Cosider oliear Volterra itegro-differetial equatio u (x) = xe x2 x x + xte u2 (t) dt, u() = With the exact solutio u(x) = x. Applyig L x (. ) = (. )dx i both sides give, u(x) = L ( 2 x + xe x2 2 Usig the method (MDAR) we get ) + L x xte u2 (t) dt x = a x = L = b x + L m= = c m, x m t = A t dt

9 Modified decompositio method by Adomia ad Rach 65 the = = x a x = L b x + L m= x m t c m,v A v dt So that b = x m++2 v= = a x = = + x+ + m= = c (+)(m++2) v= m,v A v a + a x + Where b =2 a x = b x + =2 x m+ b x x + =2 c,v A v 2 ( ) m= =2 c m,v A v 2 ( )(m+) 2 v= = x = L ( xe x2 x + ) = x x e x2 = x 8 x x6 96 x x + Equatig coefficiets b = b = b 2 = b 3 = 2 b 4 = 2 v= + b 5 = 4 m= Sice = c m, x m t = xt, we have c, = c, = c m,=, m, Therefore a = a = b a = b + 2 c ( ) v=,v. A v 2, 2 a +m =, 2, m Or a = a = b = a 2 = b + c,a = 2 2 a 3 = b 2 + c,a +c, A = 3 6 a 4 = b 3 + c,a 2 +c, A +c,2 A = 4 2 8

10 66 M. Al-Mazmumy ad S. O. Almuhalbedi The the series solutios ca be writte as u(x) = a x = x 8 x x6 96 x8 + = 48 x +.. The results produced by the preset method with oly few compoets (m=) are i a very good agreemet with the best of the results of the methods listed i Table. The preset method solutio compared with exact solutio i Figure (). x Exact (MDAR) Error....e e e e e e-3 Table (): compariso betwee exact solutio ad approximate solutio usig method Figure : compariso betwee exact solutio ad approximate solutio usig method (MDAR) Example 2.4 cosider the system of oliear Volterra itegro-differetial equatio u (x) = x + 2 x2 2 x4 x + ((x t)u 2 (t) + v 2 (t))dt, u() = v (t) = x 3 2 x2 2 x4 x + u 2 (t) + (x t)v 2 (t))dt, v() = With the exact solutio are ( + x, x). Applyig L x (. ) = (. )dx

11 Modified decompositio method by Adomia ad Rach 67 u(x) = + x 2 x2 + 6 x3 6 x5 + L x ((x t)u2 (t) + v2 (t))dt, v(x) = x 2 x2 2 x3 6 x5 + L x (u 2 (t) + (x t)v 2 (t))dt, Usig the method (MDAR) we get = a x = + L b x + L x (= t ( m= x m = v= c m,v A v + B ))dt g x = + L R x + L x = = ( t (A m= x m = c m,v B v ))dt therefore a + a x + ad g + g x + =2 =2 a x = + b x + = x + m= + x ( =2 b v= 2 c ( )(+m) m,va v 2 x m + B ( ) 2) v= R g x = + R x + = x + + =2 x ( A ( ) 2 m= 2 c ( )(+m) m,vb v 2 x m ) v= Where = b x 6 x5, equatig coefficiets = x 2 x2 + 6 x3 6 x5, ad = R x = x 2 x2 2 x3 b = b = b 2 = 2 b 3 = b 4 = 2 b =, 5, R = R = R 2 = 3 2 R 3 = R 4 = 2 R =, 5 =2 m= c, = c, = c m, =, m, 2 Sice c m, x m t = x t, we have we ow get the recursive relatio a = a = b a = b + ( 2 c ( ) v=,v A v 2 + B 2 ), 2 a +m =, 2, m

12 68 M. Al-Mazmumy ad S. O. Almuhalbedi ad g = g = R g = R + (A ( ) 2 2 v= c,v B v 2 ), 2 g +m =, 2, m Or a = a = b = a 2 = 2 b + 2 (c,a + B ) = a 3 = 3 b (c,a + c, A + B ) = a 4 = 4 b (c,a 2 + c, A + c,2 A + B 2 ) = 2 a 5 = b (c 2,A 3 + c, A 2 + c,2 A + c,3 A + B 3 ) = 5 ad g = g = R = g 2 = 2 R + 2 (A c, B ) = g 3 = 3 R (A c, B c, B ) = g 4 = 4 R (A 2 c, B 2 c, B c,2 B ) = 2 g 5 = 5 R (A 3 c, B 3 c, B 2 c,2 B ) = the the series solutio ca be writte as u(x) = = a x = a + a x + a 2 x = + x 3 x3 v(x) = = g x = g + g x + gx 2 + = x 3 2 x4 + 2 x4 5 x5 + The results produced by the preset method with oly few compoets (m=5) are i a very good agreemet with the best of the results of the methods listed i Table (2-a) ad (2-b). The (MDAR) solutio compared with exact solutio i Figure (2-a) ad Figure (2-b). x Exact (MDAR) Error....e e e e e e-2 Table (2-a): compariso betwee exact solutio u(x) ad Approximate Solutio usig method (MDAR)

13 Modified decompositio method by Adomia ad Rach 69 Figure (2-a): compariso betwee exact solutio u(x) ad Approximate Solutio usig method(mdar) x Exact M Error....e e e e e e-3 Table (2-b): compariso betwee exact solutio v(x) ad Approximate. Solutio usig method (MDAR) Figure (2-b): compariso betwee exact solutio v(x) ad Approximate. Solutio usig method (MDAR) 4. Coclusio I this study, the modificatio of Adomia ad Rach was applied to Volterra itegro-differetial equatios. We obtaied accurate approximatio aalytical solutio for Volterra itegro-differetial equatios ad the system of Volterra itegro-differetial equatios. Refereces [] R. Rach, G. Adomia, Multiple Decompositios for Computatioal Coveiece, Appl. Math. Lett., 3 (99), o. 3,

14 7 M. Al-Mazmumy ad S. O. Almuhalbedi [2] R. Rach, G. Adomia, Trasformatio of Series, Appl. Math. Lett., 4 (99), o. 4, 69-7l. [3] R. Rach, G. Adomia, Noliear Trasformatio of Series- PART II, Computers Math. Appl., 23 (992), o., [4] R. Rach, G. Adomia ad R. E. Meyers, A modified Decompositio, Computers Math. Appl., 23 (992), [5] G. Adomia ad R. Rach, Ihomogeeous oliear partial differetial equatios with variable coefficiets, Appl. Math. Lett., 5 (992), [6] G. Adomia ad R. Rach, Modified Decompositio Solutio of oliear partial differetial equatios, Appl. Math. Lett., 5 (992), [7] Lazhar Bougoffa, Solvability of the predator ad prey system with variable coefficiets ad compariso of the results with modified decompositio, Applied Mathematics ad Computatio, 82 (26), o, [8] M. Almazmumy, F. A. Hedi, H. O. Bakodah, H. Alzumi, Recet Modificatios of Adomia Decompositio Method for Iitial Value Problem i Ordiary Differetial Equatios, America Joural of Computatioal Mathematics, 2 (22), Received: Jauary 2, 27; Published: February 28, 27

Comparison Study of Series Approximation. and Convergence between Chebyshev. and Legendre Series

Comparison Study of Series Approximation. and Convergence between Chebyshev. and Legendre Series Applied Mathematical Scieces, Vol. 7, 03, o. 6, 3-337 HIKARI Ltd, www.m-hikari.com http://d.doi.org/0.988/ams.03.3430 Compariso Study of Series Approimatio ad Covergece betwee Chebyshev ad Legedre Series

More information

Similarity Solutions to Unsteady Pseudoplastic. Flow Near a Moving Wall

Similarity Solutions to Unsteady Pseudoplastic. Flow Near a Moving Wall Iteratioal Mathematical Forum, Vol. 9, 04, o. 3, 465-475 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.988/imf.04.48 Similarity Solutios to Usteady Pseudoplastic Flow Near a Movig Wall W. Robi Egieerig

More information

Taylor polynomial solution of difference equation with constant coefficients via time scales calculus

Taylor polynomial solution of difference equation with constant coefficients via time scales calculus TMSCI 3, o 3, 129-135 (2015) 129 ew Treds i Mathematical Scieces http://wwwtmscicom Taylor polyomial solutio of differece equatio with costat coefficiets via time scales calculus Veysel Fuat Hatipoglu

More information

Exact Solutions for a Class of Nonlinear Singular Two-Point Boundary Value Problems: The Decomposition Method

Exact Solutions for a Class of Nonlinear Singular Two-Point Boundary Value Problems: The Decomposition Method Exact Solutios for a Class of Noliear Sigular Two-Poit Boudary Value Problems: The Decompositio Method Abd Elhalim Ebaid Departmet of Mathematics, Faculty of Sciece, Tabuk Uiversity, P O Box 741, Tabuki

More information

Solution of Differential Equation from the Transform Technique

Solution of Differential Equation from the Transform Technique Iteratioal Joural of Computatioal Sciece ad Mathematics ISSN 0974-3189 Volume 3, Number 1 (2011), pp 121-125 Iteratioal Research Publicatio House http://wwwirphousecom Solutio of Differetial Equatio from

More information

A comparative study of a system of Lotka-Voltera type of PDEs through perturbation methods

A comparative study of a system of Lotka-Voltera type of PDEs through perturbation methods Computatioal Ecology ad Software, 13, 3(4): 11-15 Article A comparative study of a system of Lotka-Voltera type of PDEs through perturbatio methods H. A. Wahab 1, M. Shakil 1, T. Kha 1, S. Bhatti, M. Naeem

More information

Research Article A New Second-Order Iteration Method for Solving Nonlinear Equations

Research Article A New Second-Order Iteration Method for Solving Nonlinear Equations Abstract ad Applied Aalysis Volume 2013, Article ID 487062, 4 pages http://dx.doi.org/10.1155/2013/487062 Research Article A New Secod-Order Iteratio Method for Solvig Noliear Equatios Shi Mi Kag, 1 Arif

More information

The Adomian Polynomials and the New Modified Decomposition Method for BVPs of nonlinear ODEs

The Adomian Polynomials and the New Modified Decomposition Method for BVPs of nonlinear ODEs Mathematical Computatio March 015, Volume, Issue 1, PP.1 6 The Adomia Polyomials ad the New Modified Decompositio Method for BVPs of oliear ODEs Jusheg Dua # School of Scieces, Shaghai Istitute of Techology,

More information

A Taylor Series Based Method for Solving a Two-dimensional Second-order Equation

A Taylor Series Based Method for Solving a Two-dimensional Second-order Equation Applied Mathematical Scieces, Vol. 8, 2014, o. 66, 3255-3261 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2014.45347 A Taylor Series Based Method for Solvig a Two-dimesioal Secod-order Equatio

More information

Chapter 10: Power Series

Chapter 10: Power Series Chapter : Power Series 57 Chapter Overview: Power Series The reaso series are part of a Calculus course is that there are fuctios which caot be itegrated. All power series, though, ca be itegrated because

More information

Bounds for the Positive nth-root of Positive Integers

Bounds for the Positive nth-root of Positive Integers Pure Mathematical Scieces, Vol. 6, 07, o., 47-59 HIKARI Ltd, www.m-hikari.com https://doi.org/0.988/pms.07.7 Bouds for the Positive th-root of Positive Itegers Rachid Marsli Mathematics ad Statistics Departmet

More information

Higher-order iterative methods by using Householder's method for solving certain nonlinear equations

Higher-order iterative methods by using Householder's method for solving certain nonlinear equations Math Sci Lett, No, 7- ( 7 Mathematical Sciece Letters A Iteratioal Joural http://dxdoiorg/785/msl/5 Higher-order iterative methods by usig Householder's method for solvig certai oliear equatios Waseem

More information

A New Hybrid in the Nonlinear Part of Adomian Decomposition Method for Initial Value Problem of Ordinary Differential Equation

A New Hybrid in the Nonlinear Part of Adomian Decomposition Method for Initial Value Problem of Ordinary Differential Equation Joural of Matematics Researc; Vol No ; ISSN - E-ISSN - Publised b Caadia Ceter of Sciece ad Educatio A New Hbrid i te Noliear Part of Adomia Decompositio Metod for Iitial Value Problem of Ordiar Differetial

More information

arxiv: v1 [cs.sc] 2 Jan 2018

arxiv: v1 [cs.sc] 2 Jan 2018 Computig the Iverse Melli Trasform of Holoomic Sequeces usig Kovacic s Algorithm arxiv:8.9v [cs.sc] 2 Ja 28 Research Istitute for Symbolic Computatio RISC) Johaes Kepler Uiversity Liz, Alteberger Straße

More information

New Inequalities of Hermite-Hadamard-like Type for Functions whose Second Derivatives in Absolute Value are Convex

New Inequalities of Hermite-Hadamard-like Type for Functions whose Second Derivatives in Absolute Value are Convex It. Joural of Math. Aalysis, Vol. 8, 1, o. 16, 777-791 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.1988/ijma.1.1 New Ieualities of Hermite-Hadamard-like Type for Fuctios whose Secod Derivatives i

More information

Some New Iterative Methods for Solving Nonlinear Equations

Some New Iterative Methods for Solving Nonlinear Equations World Applied Scieces Joural 0 (6): 870-874, 01 ISSN 1818-495 IDOSI Publicatios, 01 DOI: 10.589/idosi.wasj.01.0.06.830 Some New Iterative Methods for Solvig Noliear Equatios Muhammad Aslam Noor, Khalida

More information

We are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n

We are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n Review of Power Series, Power Series Solutios A power series i x - a is a ifiite series of the form c (x a) =c +c (x a)+(x a) +... We also call this a power series cetered at a. Ex. (x+) is cetered at

More information

The Sampling Distribution of the Maximum. Likelihood Estimators for the Parameters of. Beta-Binomial Distribution

The Sampling Distribution of the Maximum. Likelihood Estimators for the Parameters of. Beta-Binomial Distribution Iteratioal Mathematical Forum, Vol. 8, 2013, o. 26, 1263-1277 HIKARI Ltd, www.m-hikari.com http://d.doi.org/10.12988/imf.2013.3475 The Samplig Distributio of the Maimum Likelihood Estimators for the Parameters

More information

DECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS. Park Road, Islamabad, Pakistan

DECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS. Park Road, Islamabad, Pakistan Mathematical ad Computatioal Applicatios, Vol. 9, No. 3, pp. 30-40, 04 DECOMPOSITION METHOD FOR SOLVING A SYSTEM OF THIRD-ORDER BOUNDARY VALUE PROBLEMS Muhammad Aslam Noor, Khalida Iayat Noor ad Asif Waheed

More information

Recurrence Relations

Recurrence Relations Recurrece Relatios Aalysis of recursive algorithms, such as: it factorial (it ) { if (==0) retur ; else retur ( * factorial(-)); } Let t be the umber of multiplicatios eeded to calculate factorial(). The

More information

POWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS

POWER SERIES SOLUTION OF FIRST ORDER MATRIX DIFFERENTIAL EQUATIONS Joural of Applied Mathematics ad Computatioal Mechaics 4 3(3) 3-8 POWER SERIES SOLUION OF FIRS ORDER MARIX DIFFERENIAL EQUAIONS Staisław Kukla Izabela Zamorska Istitute of Mathematics Czestochowa Uiversity

More information

NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE

NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE UPB Sci Bull, Series A, Vol 79, Iss, 207 ISSN 22-7027 NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE Gabriel Bercu We itroduce two ew sequeces of Euler-Mascheroi type which have fast covergece

More information

Convergence of Random SP Iterative Scheme

Convergence of Random SP Iterative Scheme Applied Mathematical Scieces, Vol. 7, 2013, o. 46, 2283-2293 HIKARI Ltd, www.m-hikari.com Covergece of Radom SP Iterative Scheme 1 Reu Chugh, 2 Satish Narwal ad 3 Vivek Kumar 1,2,3 Departmet of Mathematics,

More information

A NEW CLASS OF 2-STEP RATIONAL MULTISTEP METHODS

A NEW CLASS OF 2-STEP RATIONAL MULTISTEP METHODS Jural Karya Asli Loreka Ahli Matematik Vol. No. (010) page 6-9. Jural Karya Asli Loreka Ahli Matematik A NEW CLASS OF -STEP RATIONAL MULTISTEP METHODS 1 Nazeeruddi Yaacob Teh Yua Yig Norma Alias 1 Departmet

More information

CHAPTER 10 INFINITE SEQUENCES AND SERIES

CHAPTER 10 INFINITE SEQUENCES AND SERIES CHAPTER 10 INFINITE SEQUENCES AND SERIES 10.1 Sequeces 10.2 Ifiite Series 10.3 The Itegral Tests 10.4 Compariso Tests 10.5 The Ratio ad Root Tests 10.6 Alteratig Series: Absolute ad Coditioal Covergece

More information

wavelet collocation method for solving integro-differential equation.

wavelet collocation method for solving integro-differential equation. IOSR Joural of Egieerig (IOSRJEN) ISSN (e): 5-3, ISSN (p): 78-879 Vol. 5, Issue 3 (arch. 5), V3 PP -7 www.iosrje.org wavelet collocatio method for solvig itegro-differetial equatio. Asmaa Abdalelah Abdalrehma

More information

COMPLEX FACTORIZATIONS OF THE GENERALIZED FIBONACCI SEQUENCES {q n } Sang Pyo Jun

COMPLEX FACTORIZATIONS OF THE GENERALIZED FIBONACCI SEQUENCES {q n } Sang Pyo Jun Korea J. Math. 23 2015) No. 3 pp. 371 377 http://dx.doi.org/10.11568/kjm.2015.23.3.371 COMPLEX FACTORIZATIONS OF THE GENERALIZED FIBONACCI SEQUENCES {q } Sag Pyo Ju Abstract. I this ote we cosider a geeralized

More information

A collocation method for singular integral equations with cosecant kernel via Semi-trigonometric interpolation

A collocation method for singular integral equations with cosecant kernel via Semi-trigonometric interpolation Iteratioal Joural of Mathematics Research. ISSN 0976-5840 Volume 9 Number 1 (017) pp. 45-51 Iteratioal Research Publicatio House http://www.irphouse.com A collocatio method for sigular itegral equatios

More information

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 +

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + 62. Power series Defiitio 16. (Power series) Give a sequece {c }, the series c x = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + is called a power series i the variable x. The umbers c are called the coefficiets of

More information

SOLUTIONS TO EXAM 3. Solution: Note that this defines two convergent geometric series with respective radii r 1 = 2/5 < 1 and r 2 = 1/5 < 1.

SOLUTIONS TO EXAM 3. Solution: Note that this defines two convergent geometric series with respective radii r 1 = 2/5 < 1 and r 2 = 1/5 < 1. SOLUTIONS TO EXAM 3 Problem Fid the sum of the followig series 2 + ( ) 5 5 2 5 3 25 2 2 This series diverges Solutio: Note that this defies two coverget geometric series with respective radii r 2/5 < ad

More information

EXACT SOLUTION OF WHITHAM-BROER-KAUP SHALLOW WATER WAVE EQUATIONS

EXACT SOLUTION OF WHITHAM-BROER-KAUP SHALLOW WATER WAVE EQUATIONS Joural of Sciece ad Arts Year 5, No. (3), pp. 5-, 5 ORIGINAL PAPER EXACT SOLUTION OF WHITHAM-BROER-KAUP SHALLOW WATER WAVE EQUATIONS JAMSHAD AHMAD, MARIYAM MUSHTAQ, NADEEM SAJJAD 3 Mauscript received:

More information

Exact Solutions of the Generalized Benjamin Equation and (3 + 1)- Dimensional Gkp Equation by the Extended Tanh Method

Exact Solutions of the Generalized Benjamin Equation and (3 + 1)- Dimensional Gkp Equation by the Extended Tanh Method Available at http://pvamuedu/aam Appl Appl Math ISSN: 93-9466 Vol 7, Issue (Jue 0), pp 75 87 Applicatios ad Applied Mathematics: A Iteratioal Joural (AAM) Exact Solutios of the Geeralized Bejami Equatio

More information

Generating Functions for Laguerre Type Polynomials. Group Theoretic method

Generating Functions for Laguerre Type Polynomials. Group Theoretic method It. Joural of Math. Aalysis, Vol. 4, 2010, o. 48, 257-266 Geeratig Fuctios for Laguerre Type Polyomials α of Two Variables L ( xy, ) by Usig Group Theoretic method Ajay K. Shula* ad Sriata K. Meher** *Departmet

More information

On Generalized Fibonacci Numbers

On Generalized Fibonacci Numbers Applied Mathematical Scieces, Vol. 9, 215, o. 73, 3611-3622 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.12988/ams.215.5299 O Geeralized Fiboacci Numbers Jerico B. Bacai ad Julius Fergy T. Rabago Departmet

More information

NICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) =

NICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) = AN INTRODUCTION TO SCHRÖDER AND UNKNOWN NUMBERS NICK DUFRESNE Abstract. I this article we will itroduce two types of lattice paths, Schröder paths ad Ukow paths. We will examie differet properties of each,

More information

Discrete Orthogonal Moment Features Using Chebyshev Polynomials

Discrete Orthogonal Moment Features Using Chebyshev Polynomials Discrete Orthogoal Momet Features Usig Chebyshev Polyomials R. Mukuda, 1 S.H.Og ad P.A. Lee 3 1 Faculty of Iformatio Sciece ad Techology, Multimedia Uiversity 75450 Malacca, Malaysia. Istitute of Mathematical

More information

Newton Homotopy Solution for Nonlinear Equations Using Maple14. Abstract

Newton Homotopy Solution for Nonlinear Equations Using Maple14. Abstract Joural of Sciece ad Techology ISSN 9-860 Vol. No. December 0 Newto Homotopy Solutio for Noliear Equatios Usig Maple Nor Haim Abd. Rahma, Arsmah Ibrahim, Mohd Idris Jayes Faculty of Computer ad Mathematical

More information

Numerical Solutions of Second Order Boundary Value Problems by Galerkin Residual Method on Using Legendre Polynomials

Numerical Solutions of Second Order Boundary Value Problems by Galerkin Residual Method on Using Legendre Polynomials IOSR Joural of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 319-765X. Volume 11, Issue 6 Ver. IV (Nov. - Dec. 15), PP 1-11 www.iosrjourals.org Numerical Solutios of Secod Order Boudary Value Problems

More information

On the Derivation and Implementation of a Four Stage Harmonic Explicit Runge-Kutta Method *

On the Derivation and Implementation of a Four Stage Harmonic Explicit Runge-Kutta Method * Applied Mathematics, 05, 6, 694-699 Published Olie April 05 i SciRes. http://www.scirp.org/joural/am http://dx.doi.org/0.46/am.05.64064 O the Derivatio ad Implemetatio of a Four Stage Harmoic Explicit

More information

The Differential Transform Method for Solving Volterra s Population Model

The Differential Transform Method for Solving Volterra s Population Model AASCIT Couicatios Volue, Issue 6 Septeber, 15 olie ISSN: 375-383 The Differetial Trasfor Method for Solvig Volterra s Populatio Model Khatereh Tabatabaei Departet of Matheatics, Faculty of Sciece, Kafas

More information

Mathematics review for CSCI 303 Spring Department of Computer Science College of William & Mary Robert Michael Lewis

Mathematics review for CSCI 303 Spring Department of Computer Science College of William & Mary Robert Michael Lewis Mathematics review for CSCI 303 Sprig 019 Departmet of Computer Sciece College of William & Mary Robert Michael Lewis Copyright 018 019 Robert Michael Lewis Versio geerated: 13 : 00 Jauary 17, 019 Cotets

More information

Improved Class of Ratio -Cum- Product Estimators of Finite Population Mean in two Phase Sampling

Improved Class of Ratio -Cum- Product Estimators of Finite Population Mean in two Phase Sampling Global Joural of Sciece Frotier Research: F Mathematics ad Decisio Scieces Volume 4 Issue 2 Versio.0 Year 204 Type : Double Blid Peer Reviewed Iteratioal Research Joural Publisher: Global Jourals Ic. (USA

More information

New Results for the Fibonacci Sequence Using Binet s Formula

New Results for the Fibonacci Sequence Using Binet s Formula Iteratioal Mathematical Forum, Vol. 3, 208, o. 6, 29-266 HIKARI Ltd, www.m-hikari.com https://doi.org/0.2988/imf.208.832 New Results for the Fiboacci Sequece Usig Biet s Formula Reza Farhadia Departmet

More information

MTH 142 Exam 3 Spr 2011 Practice Problem Solutions 1

MTH 142 Exam 3 Spr 2011 Practice Problem Solutions 1 MTH 42 Exam 3 Spr 20 Practice Problem Solutios No calculators will be permitted at the exam. 3. A pig-pog ball is lauched straight up, rises to a height of 5 feet, the falls back to the lauch poit ad bouces

More information

ENGI Series Page 6-01

ENGI Series Page 6-01 ENGI 3425 6 Series Page 6-01 6. Series Cotets: 6.01 Sequeces; geeral term, limits, covergece 6.02 Series; summatio otatio, covergece, divergece test 6.03 Stadard Series; telescopig series, geometric series,

More information

Research Article Some E-J Generalized Hausdorff Matrices Not of Type M

Research Article Some E-J Generalized Hausdorff Matrices Not of Type M Abstract ad Applied Aalysis Volume 2011, Article ID 527360, 5 pages doi:10.1155/2011/527360 Research Article Some E-J Geeralized Hausdorff Matrices Not of Type M T. Selmaogullari, 1 E. Savaş, 2 ad B. E.

More information

Chapter 4 : Laplace Transform

Chapter 4 : Laplace Transform 4. Itroductio Laplace trasform is a alterative to solve the differetial equatio by the complex frequecy domai ( s = σ + jω), istead of the usual time domai. The DE ca be easily trasformed ito a algebraic

More information

THE NUMERICAL SOLUTION OF THE NEWTONIAN FLUIDS FLOW DUE TO A STRETCHING CYLINDER BY SOR ITERATIVE PROCEDURE ABSTRACT

THE NUMERICAL SOLUTION OF THE NEWTONIAN FLUIDS FLOW DUE TO A STRETCHING CYLINDER BY SOR ITERATIVE PROCEDURE ABSTRACT Europea Joural of Egieerig ad Techology Vol. 3 No., 5 ISSN 56-586 THE NUMERICAL SOLUTION OF THE NEWTONIAN FLUIDS FLOW DUE TO A STRETCHING CYLINDER BY SOR ITERATIVE PROCEDURE Atif Nazir, Tahir Mahmood ad

More information

-ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION

-ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION NEW NEWTON-TYPE METHOD WITH k -ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION R. Thukral Padé Research Cetre, 39 Deaswood Hill, Leeds West Yorkshire, LS7 JS, ENGLAND ABSTRACT The objective

More information

μ are complex parameters. Other

μ are complex parameters. Other A New Numerical Itegrator for the Solutio of Iitial Value Problems i Ordiary Differetial Equatios. J. Suday * ad M.R. Odekule Departmet of Mathematical Scieces, Adamawa State Uiversity, Mubi, Nigeria.

More information

You may work in pairs or purely individually for this assignment.

You may work in pairs or purely individually for this assignment. CS 04 Problem Solvig i Computer Sciece OOC Assigmet 6: Recurreces You may work i pairs or purely idividually for this assigmet. Prepare your aswers to the followig questios i a plai ASCII text file or

More information

Some properties of Boubaker polynomials and applications

Some properties of Boubaker polynomials and applications Some properties of Boubaker polyomials ad applicatios Gradimir V. Milovaović ad Duša Joksimović Citatio: AIP Cof. Proc. 179, 1050 (2012); doi: 10.1063/1.756326 View olie: http://dx.doi.org/10.1063/1.756326

More information

Uniform Strict Practical Stability Criteria for Impulsive Functional Differential Equations

Uniform Strict Practical Stability Criteria for Impulsive Functional Differential Equations Global Joural of Sciece Frotier Research Mathematics ad Decisio Scieces Volume 3 Issue Versio 0 Year 03 Type : Double Blid Peer Reviewed Iteratioal Research Joural Publisher: Global Jourals Ic (USA Olie

More information

Weakly Connected Closed Geodetic Numbers of Graphs

Weakly Connected Closed Geodetic Numbers of Graphs Iteratioal Joural of Mathematical Aalysis Vol 10, 016, o 6, 57-70 HIKARI Ltd, wwwm-hikaricom http://dxdoiorg/101988/ijma01651193 Weakly Coected Closed Geodetic Numbers of Graphs Rachel M Pataga 1, Imelda

More information

Review Article Incomplete Bivariate Fibonacci and Lucas p-polynomials

Review Article Incomplete Bivariate Fibonacci and Lucas p-polynomials Discrete Dyamics i Nature ad Society Volume 2012, Article ID 840345, 11 pages doi:10.1155/2012/840345 Review Article Icomplete Bivariate Fiboacci ad Lucas p-polyomials Dursu Tasci, 1 Mirac Ceti Firegiz,

More information

The Riemann Zeta Function

The Riemann Zeta Function Physics 6A Witer 6 The Riema Zeta Fuctio I this ote, I will sketch some of the mai properties of the Riema zeta fuctio, ζ(x). For x >, we defie ζ(x) =, x >. () x = For x, this sum diverges. However, we

More information

PAijpam.eu ON TENSOR PRODUCT DECOMPOSITION

PAijpam.eu ON TENSOR PRODUCT DECOMPOSITION Iteratioal Joural of Pure ad Applied Mathematics Volume 103 No 3 2015, 537-545 ISSN: 1311-8080 (prited versio); ISSN: 1314-3395 (o-lie versio) url: http://wwwijpameu doi: http://dxdoiorg/1012732/ijpamv103i314

More information

Bangi 43600, Selangor Darul Ehsan, Malaysia (Received 12 February 2010, accepted 21 April 2010)

Bangi 43600, Selangor Darul Ehsan, Malaysia (Received 12 February 2010, accepted 21 April 2010) O Cesáro Meas of Order μ for Outer Fuctios ISSN 1749-3889 (prit), 1749-3897 (olie) Iteratioal Joural of Noliear Sciece Vol9(2010) No4,pp455-460 Maslia Darus 1, Rabha W Ibrahim 2 1,2 School of Mathematical

More information

Some Variants of Newton's Method with Fifth-Order and Fourth-Order Convergence for Solving Nonlinear Equations

Some Variants of Newton's Method with Fifth-Order and Fourth-Order Convergence for Solving Nonlinear Equations Copyright, Darbose Iteratioal Joural o Applied Mathematics ad Computatio Volume (), pp -6, 9 http//: ijamc.darbose.com Some Variats o Newto's Method with Fith-Order ad Fourth-Order Covergece or Solvig

More information

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense, 3. Z Trasform Referece: Etire Chapter 3 of text. Recall that the Fourier trasform (FT) of a DT sigal x [ ] is ω ( ) [ ] X e = j jω k = xe I order for the FT to exist i the fiite magitude sese, S = x [

More information

ECE-S352 Introduction to Digital Signal Processing Lecture 3A Direct Solution of Difference Equations

ECE-S352 Introduction to Digital Signal Processing Lecture 3A Direct Solution of Difference Equations ECE-S352 Itroductio to Digital Sigal Processig Lecture 3A Direct Solutio of Differece Equatios Discrete Time Systems Described by Differece Equatios Uit impulse (sample) respose h() of a DT system allows

More information

NTMSCI 5, No. 1, (2017) 26

NTMSCI 5, No. 1, (2017) 26 NTMSCI 5, No. 1, - (17) New Treds i Mathematical Scieces http://dx.doi.org/1.85/tmsci.17.1 The geeralized successive approximatio ad Padé approximats method for solvig a elasticity problem of based o the

More information

Math 113 Exam 3 Practice

Math 113 Exam 3 Practice Math Exam Practice Exam 4 will cover.-., 0. ad 0.. Note that eve though. was tested i exam, questios from that sectios may also be o this exam. For practice problems o., refer to the last review. This

More information

TR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT

TR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT TR/46 OCTOBER 974 THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION by A. TALBOT .. Itroductio. A problem i approximatio theory o which I have recetly worked [] required for its solutio a proof that the

More information

1 6 = 1 6 = + Factorials and Euler s Gamma function

1 6 = 1 6 = + Factorials and Euler s Gamma function Royal Holloway Uiversity of Lodo Departmet of Physics Factorials ad Euler s Gamma fuctio Itroductio The is a self-cotaied part of the course dealig, essetially, with the factorial fuctio ad its geeralizatio

More information

Double Stage Shrinkage Estimator of Two Parameters. Generalized Exponential Distribution

Double Stage Shrinkage Estimator of Two Parameters. Generalized Exponential Distribution Iteratioal Mathematical Forum, Vol., 3, o. 3, 3-53 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.9/imf.3.335 Double Stage Shrikage Estimator of Two Parameters Geeralized Expoetial Distributio Alaa M.

More information

Math 12 Final Exam, May 11, 2011 ANSWER KEY. 2sinh(2x) = lim. 1 x. lim e. x ln. = e. (x+1)(1) x(1) (x+1) 2. (2secθ) 5 2sec2 θ dθ.

Math 12 Final Exam, May 11, 2011 ANSWER KEY. 2sinh(2x) = lim. 1 x. lim e. x ln. = e. (x+1)(1) x(1) (x+1) 2. (2secθ) 5 2sec2 θ dθ. Math Fial Exam, May, ANSWER KEY. [5 Poits] Evaluate each of the followig its. Please justify your aswers. Be clear if the it equals a value, + or, or Does Not Exist. coshx) a) L H x x+l x) sihx) x x L

More information

k-generalized FIBONACCI NUMBERS CLOSE TO THE FORM 2 a + 3 b + 5 c 1. Introduction

k-generalized FIBONACCI NUMBERS CLOSE TO THE FORM 2 a + 3 b + 5 c 1. Introduction Acta Math. Uiv. Comeiaae Vol. LXXXVI, 2 (2017), pp. 279 286 279 k-generalized FIBONACCI NUMBERS CLOSE TO THE FORM 2 a + 3 b + 5 c N. IRMAK ad M. ALP Abstract. The k-geeralized Fiboacci sequece { F (k)

More information

Reconstruction of the Volterra-type integro-differential operator from nodal points

Reconstruction of the Volterra-type integro-differential operator from nodal points Keski Boudary Value Problems 18 18:47 https://doi.org/1.1186/s13661-18-968- R E S E A R C H Ope Access Recostructio of the Volterra-type itegro-differetial operator from odal poits Baki Keski * * Correspodece:

More information

LOWER BOUNDS FOR THE BLOW-UP TIME OF NONLINEAR PARABOLIC PROBLEMS WITH ROBIN BOUNDARY CONDITIONS

LOWER BOUNDS FOR THE BLOW-UP TIME OF NONLINEAR PARABOLIC PROBLEMS WITH ROBIN BOUNDARY CONDITIONS Electroic Joural of Differetial Equatios, Vol. 214 214), No. 113, pp. 1 5. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.ut.edu ftp ejde.math.txstate.edu LOWER BOUNDS FOR THE BLOW-UP

More information

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS MIDTERM 3 CALCULUS MATH 300 FALL 08 Moday, December 3, 08 5:5 PM to 6:45 PM Name PRACTICE EXAM S Please aswer all of the questios, ad show your work. You must explai your aswers to get credit. You will

More information

Solving a Nonlinear Equation Using a New Two-Step Derivative Free Iterative Methods

Solving a Nonlinear Equation Using a New Two-Step Derivative Free Iterative Methods Applied ad Computatioal Mathematics 07; 6(6): 38-4 http://www.sciecepublishiggroup.com/j/acm doi: 0.648/j.acm.070606. ISSN: 38-5605 (Prit); ISSN: 38-563 (Olie) Solvig a Noliear Equatio Usig a New Two-Step

More information

Research Article Two Expanding Integrable Models of the Geng-Cao Hierarchy

Research Article Two Expanding Integrable Models of the Geng-Cao Hierarchy Abstract ad Applied Aalysis Volume 214, Article ID 86935, 7 pages http://d.doi.org/1.1155/214/86935 Research Article Two Epadig Itegrable Models of the Geg-Cao Hierarchy Xiurog Guo, 1 Yufeg Zhag, 2 ad

More information

Research Article Nonexistence of Homoclinic Solutions for a Class of Discrete Hamiltonian Systems

Research Article Nonexistence of Homoclinic Solutions for a Class of Discrete Hamiltonian Systems Abstract ad Applied Aalysis Volume 203, Article ID 39868, 6 pages http://dx.doi.org/0.55/203/39868 Research Article Noexistece of Homocliic Solutios for a Class of Discrete Hamiltoia Systems Xiaopig Wag

More information

Math 113 Exam 3 Practice

Math 113 Exam 3 Practice Math Exam Practice Exam will cover.-.9. This sheet has three sectios. The first sectio will remid you about techiques ad formulas that you should kow. The secod gives a umber of practice questios for you

More information

Gaps between Consecutive Perfect Powers

Gaps between Consecutive Perfect Powers Iteratioal Mathematical Forum, Vol. 11, 016, o. 9, 49-437 HIKARI Lt, www.m-hikari.com http://x.oi.org/10.1988/imf.016.63 Gaps betwee Cosecutive Perfect Powers Rafael Jakimczuk Divisió Matemática, Uiversia

More information

SOLUTION SET VI FOR FALL [(n + 2)(n + 1)a n+2 a n 1 ]x n = 0,

SOLUTION SET VI FOR FALL [(n + 2)(n + 1)a n+2 a n 1 ]x n = 0, 4. Series Solutios of Differetial Equatios:Special Fuctios 4.. Illustrative examples.. 5. Obtai the geeral solutio of each of the followig differetial equatios i terms of Maclauri series: d y (a dx = xy,

More information

1. Linearization of a nonlinear system given in the form of a system of ordinary differential equations

1. Linearization of a nonlinear system given in the form of a system of ordinary differential equations . Liearizatio of a oliear system give i the form of a system of ordiary differetial equatios We ow show how to determie a liear model which approximates the behavior of a time-ivariat oliear system i a

More information

PLEASE MARK YOUR ANSWERS WITH AN X, not a circle! 1. (a) (b) (c) (d) (e) 3. (a) (b) (c) (d) (e) 5. (a) (b) (c) (d) (e) 7. (a) (b) (c) (d) (e)

PLEASE MARK YOUR ANSWERS WITH AN X, not a circle! 1. (a) (b) (c) (d) (e) 3. (a) (b) (c) (d) (e) 5. (a) (b) (c) (d) (e) 7. (a) (b) (c) (d) (e) Math 0560, Exam 3 November 6, 07 The Hoor Code is i effect for this examiatio. All work is to be your ow. No calculators. The exam lasts for hour ad 5 mi. Be sure that your ame is o every page i case pages

More information

Sequences and Series of Functions

Sequences and Series of Functions Chapter 6 Sequeces ad Series of Fuctios 6.1. Covergece of a Sequece of Fuctios Poitwise Covergece. Defiitio 6.1. Let, for each N, fuctio f : A R be defied. If, for each x A, the sequece (f (x)) coverges

More information

Calculus 2 - D. Yuen Final Exam Review (Version 11/22/2017. Please report any possible typos.)

Calculus 2 - D. Yuen Final Exam Review (Version 11/22/2017. Please report any possible typos.) Calculus - D Yue Fial Eam Review (Versio //7 Please report ay possible typos) NOTE: The review otes are oly o topics ot covered o previous eams See previous review sheets for summary of previous topics

More information

AMS Mathematics Subject Classification : 40A05, 40A99, 42A10. Key words and phrases : Harmonic series, Fourier series. 1.

AMS Mathematics Subject Classification : 40A05, 40A99, 42A10. Key words and phrases : Harmonic series, Fourier series. 1. J. Appl. Math. & Computig Vol. x 00y), No. z, pp. A RECURSION FOR ALERNAING HARMONIC SERIES ÁRPÁD BÉNYI Abstract. We preset a coveiet recursive formula for the sums of alteratig harmoic series of odd order.

More information

Phys. 201 Mathematical Physics 1 Dr. Nidal M. Ershaidat Doc. 12

Phys. 201 Mathematical Physics 1 Dr. Nidal M. Ershaidat Doc. 12 Physics Departmet, Yarmouk Uiversity, Irbid Jorda Phys. Mathematical Physics Dr. Nidal M. Ershaidat Doc. Fourier Series Deiitio A Fourier series is a expasio o a periodic uctio (x) i terms o a iiite sum

More information

CertainSequencesanditsIntegralRepresentationsinTermsofLaguerrePolynomials

CertainSequencesanditsIntegralRepresentationsinTermsofLaguerrePolynomials Global Joural of Sciece Frotier Research: F Mathematics ad Decisio Scieces Volume 5 Issue 5 Versio. Year 5 Type : Double Blid Peer Reviewed Iteratioal Research Joural Publisher: Global Jourals Ic. USA

More information

Time-Domain Representations of LTI Systems

Time-Domain Representations of LTI Systems 2.1 Itroductio Objectives: 1. Impulse resposes of LTI systems 2. Liear costat-coefficiets differetial or differece equatios of LTI systems 3. Bloc diagram represetatios of LTI systems 4. State-variable

More information

Stability Analysis of the Euler Discretization for SIR Epidemic Model

Stability Analysis of the Euler Discretization for SIR Epidemic Model Stability Aalysis of the Euler Discretizatio for SIR Epidemic Model Agus Suryato Departmet of Mathematics, Faculty of Scieces, Brawijaya Uiversity, Jl Vetera Malag 6545 Idoesia Abstract I this paper we

More information

Research Article Approximate Riesz Algebra-Valued Derivations

Research Article Approximate Riesz Algebra-Valued Derivations Abstract ad Applied Aalysis Volume 2012, Article ID 240258, 5 pages doi:10.1155/2012/240258 Research Article Approximate Riesz Algebra-Valued Derivatios Faruk Polat Departmet of Mathematics, Faculty of

More information

Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations

Application of Homotopy Analysis Method for Solving various types of Problems of Ordinary Differential Equations Iteratioal Joural o Recet ad Iovatio Treds i Coputig ad Couicatio IN: 31-8169 Volue: 5 Issue: 5 16 Applicatio of Hootopy Aalysis Meod for olvig various types of Probles of Ordiary Differetial Equatios

More information

Sequences of Definite Integrals, Factorials and Double Factorials

Sequences of Definite Integrals, Factorials and Double Factorials 47 6 Joural of Iteger Sequeces, Vol. 8 (5), Article 5.4.6 Sequeces of Defiite Itegrals, Factorials ad Double Factorials Thierry Daa-Picard Departmet of Applied Mathematics Jerusalem College of Techology

More information

MH1101 AY1617 Sem 2. Question 1. NOT TESTED THIS TIME

MH1101 AY1617 Sem 2. Question 1. NOT TESTED THIS TIME MH AY67 Sem Questio. NOT TESTED THIS TIME ( marks Let R be the regio bouded by the curve y 4x x 3 ad the x axis i the first quadrat (see figure below. Usig the cylidrical shell method, fid the volume of

More information

Numerical Solution of the Two Point Boundary Value Problems By Using Wavelet Bases of Hermite Cubic Spline Wavelets

Numerical Solution of the Two Point Boundary Value Problems By Using Wavelet Bases of Hermite Cubic Spline Wavelets Australia Joural of Basic ad Applied Scieces, 5(): 98-5, ISSN 99-878 Numerical Solutio of the Two Poit Boudary Value Problems By Usig Wavelet Bases of Hermite Cubic Splie Wavelets Mehdi Yousefi, Hesam-Aldie

More information

ON POINTWISE BINOMIAL APPROXIMATION

ON POINTWISE BINOMIAL APPROXIMATION Iteratioal Joural of Pure ad Applied Mathematics Volume 71 No. 1 2011, 57-66 ON POINTWISE BINOMIAL APPROXIMATION BY w-functions K. Teerapabolar 1, P. Wogkasem 2 Departmet of Mathematics Faculty of Sciece

More information

ADM Solution of Flow Field and Convective Heat Transfer over a Parallel Flat Plate and Comparison with the Forth Order Runge Kutta Method

ADM Solution of Flow Field and Convective Heat Transfer over a Parallel Flat Plate and Comparison with the Forth Order Runge Kutta Method Australia Joural of Basic ad Applied Scieces, 5(: -8, ISSN 99-878 ADM Solutio of Flow Field ad Covective Heat Trasfer over a Parallel Flat Plate ad Compariso with the Forth Order Ruge Kutta Method Arma

More information

(a) (b) All real numbers. (c) All real numbers. (d) None. to show the. (a) 3. (b) [ 7, 1) (c) ( 7, 1) (d) At x = 7. (a) (b)

(a) (b) All real numbers. (c) All real numbers. (d) None. to show the. (a) 3. (b) [ 7, 1) (c) ( 7, 1) (d) At x = 7. (a) (b) Chapter 0 Review 597. E; a ( + )( + ) + + S S + S + + + + + + S lim + l. D; a diverges by the Itegral l k Test sice d lim [(l ) ], so k l ( ) does ot coverge absolutely. But it coverges by the Alteratig

More information

AH Checklist (Unit 3) AH Checklist (Unit 3) Matrices

AH Checklist (Unit 3) AH Checklist (Unit 3) Matrices AH Checklist (Uit 3) AH Checklist (Uit 3) Matrices Skill Achieved? Kow that a matrix is a rectagular array of umbers (aka etries or elemets) i paretheses, each etry beig i a particular row ad colum Kow

More information

Recursive Algorithms. Recurrences. Recursive Algorithms Analysis

Recursive Algorithms. Recurrences. Recursive Algorithms Analysis Recursive Algorithms Recurreces Computer Sciece & Egieerig 35: Discrete Mathematics Christopher M Bourke cbourke@cseuledu A recursive algorithm is oe i which objects are defied i terms of other objects

More information

Direct Estimates for Lupaş-Durrmeyer Operators

Direct Estimates for Lupaş-Durrmeyer Operators Filomat 3:1 16, 191 199 DOI 1.98/FIL161191A Published by Faculty of Scieces ad Mathematics, Uiversity of Niš, Serbia Available at: http://www.pmf.i.ac.rs/filomat Direct Estimates for Lupaş-Durrmeyer Operators

More information

MAT1026 Calculus II Basic Convergence Tests for Series

MAT1026 Calculus II Basic Convergence Tests for Series MAT026 Calculus II Basic Covergece Tests for Series Egi MERMUT 202.03.08 Dokuz Eylül Uiversity Faculty of Sciece Departmet of Mathematics İzmir/TURKEY Cotets Mootoe Covergece Theorem 2 2 Series of Real

More information

, then cv V. Differential Equations Elements of Lineaer Algebra Name: Consider the differential equation. and y2 cos( kx)

, then cv V. Differential Equations Elements of Lineaer Algebra Name: Consider the differential equation. and y2 cos( kx) Cosider the differetial equatio y '' k y 0 has particular solutios y1 si( kx) ad y cos( kx) I geeral, ay liear combiatio of y1 ad y, cy 1 1 cy where c1, c is also a solutio to the equatio above The reaso

More information

Problem Cosider the curve give parametrically as x = si t ad y = + cos t for» t» ß: (a) Describe the path this traverses: Where does it start (whe t =

Problem Cosider the curve give parametrically as x = si t ad y = + cos t for» t» ß: (a) Describe the path this traverses: Where does it start (whe t = Mathematics Summer Wilso Fial Exam August 8, ANSWERS Problem 1 (a) Fid the solutio to y +x y = e x x that satisfies y() = 5 : This is already i the form we used for a first order liear differetial equatio,

More information