On computing differential transform of nonlinear non-autonomous functions and its applications

Similar documents
Approximate Analytic Solution of (2+1) - Dimensional Zakharov-Kuznetsov(Zk) Equations Using Homotopy

HEAT CONDUCTION PROBLEM IN A TWO-LAYERED HOLLOW CYLINDER BY USING THE GREEN S FUNCTION METHOD

A NEW TECHNIQUE FOR SOLVING THE 1-D BURGERS EQUATION

GENERATING CERTAIN QUINTIC IRREDUCIBLE POLYNOMIALS OVER FINITE FIELDS. Youngwoo Ahn and Kitae Kim

On One Analytic Method of. Constructing Program Controls

Cubic Bezier Homotopy Function for Solving Exponential Equations

M. Y. Adamu Mathematical Sciences Programme, AbubakarTafawaBalewa University, Bauchi, Nigeria

Mechanics Physics 151

Relative controllability of nonlinear systems with delays in control

Existence and Uniqueness Results for Random Impulsive Integro-Differential Equation

V.Abramov - FURTHER ANALYSIS OF CONFIDENCE INTERVALS FOR LARGE CLIENT/SERVER COMPUTER NETWORKS

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

Chapter Lagrangian Interpolation

Including the ordinary differential of distance with time as velocity makes a system of ordinary differential equations.

A DECOMPOSITION METHOD FOR SOLVING DIFFUSION EQUATIONS VIA LOCAL FRACTIONAL TIME DERIVATIVE

P R = P 0. The system is shown on the next figure:

Linear Response Theory: The connection between QFT and experiments

( ) () we define the interaction representation by the unitary transformation () = ()

FTCS Solution to the Heat Equation

Method of upper lower solutions for nonlinear system of fractional differential equations and applications

[ ] 2. [ ]3 + (Δx i + Δx i 1 ) / 2. Δx i-1 Δx i Δx i+1. TPG4160 Reservoir Simulation 2018 Lecture note 3. page 1 of 5

Tight results for Next Fit and Worst Fit with resource augmentation

Research Article Numerical Approximation of Higher-Order Solutions of the Quadratic Nonlinear Stochastic Oscillatory Equation Using WHEP Technique

Lecture 18: The Laplace Transform (See Sections and 14.7 in Boas)

New M-Estimator Objective Function. in Simultaneous Equations Model. (A Comparative Study)

Survival Analysis and Reliability. A Note on the Mean Residual Life Function of a Parallel System

FI 3103 Quantum Physics

On the numerical treatment ofthenonlinear partial differentialequation of fractional order

Handout # 6 (MEEN 617) Numerical Integration to Find Time Response of SDOF mechanical system Y X (2) and write EOM (1) as two first-order Eqs.

In the complete model, these slopes are ANALYSIS OF VARIANCE FOR THE COMPLETE TWO-WAY MODEL. (! i+1 -! i ) + [(!") i+1,q - [(!

3. OVERVIEW OF NUMERICAL METHODS

Performance Analysis for a Network having Standby Redundant Unit with Waiting in Repair

Attribute Reduction Algorithm Based on Discernibility Matrix with Algebraic Method GAO Jing1,a, Ma Hui1, Han Zhidong2,b

NATIONAL UNIVERSITY OF SINGAPORE PC5202 ADVANCED STATISTICAL MECHANICS. (Semester II: AY ) Time Allowed: 2 Hours

Solution in semi infinite diffusion couples (error function analysis)

Chapter 6: AC Circuits

Solving the multi-period fixed cost transportation problem using LINGO solver

Notes on the stability of dynamic systems and the use of Eigen Values.

Implementation of Quantized State Systems in MATLAB/Simulink

FRACTIONAL OPTICAL SOLITARY WAVE SOLUTIONS OF THE HIGHER-ORDER NONLINEAR SCHRÖDINGER EQUATION

The Finite Element Method for the Analysis of Non-Linear and Dynamic Systems

Delay-Range-Dependent Stability Analysis for Continuous Linear System with Interval Delay

CS434a/541a: Pattern Recognition Prof. Olga Veksler. Lecture 4

PHYS 705: Classical Mechanics. Canonical Transformation

e-journal Reliability: Theory& Applications No 2 (Vol.2) Vyacheslav Abramov

How about the more general "linear" scalar functions of scalars (i.e., a 1st degree polynomial of the following form with a constant term )?

Ordinary Differential Equations in Neuroscience with Matlab examples. Aim 1- Gain understanding of how to set up and solve ODE s

Volatility Interpolation

First-order piecewise-linear dynamic circuits

Mohammad H. Al-Towaiq a & Hasan K. Al-Bzoor a a Department of Mathematics and Statistics, Jordan University of

Bayesian Inference of the GARCH model with Rational Errors

Generalized double sinh-gordon equation: Symmetry reductions, exact solutions and conservation laws

Robust and Accurate Cancer Classification with Gene Expression Profiling

Coupled Method for Solving Time-Fractional Navier-Stokes Equation

Comparison of Differences between Power Means 1

J i-1 i. J i i+1. Numerical integration of the diffusion equation (I) Finite difference method. Spatial Discretization. Internal nodes.

Supplementary Material to: IMU Preintegration on Manifold for E cient Visual-Inertial Maximum-a-Posteriori Estimation

A New Generalized Gronwall-Bellman Type Inequality

Let s treat the problem of the response of a system to an applied external force. Again,

Department of Economics University of Toronto

2/20/2013. EE 101 Midterm 2 Review

@FMI c Kyung Moon Sa Co.

Online Supplement for Dynamic Multi-Technology. Production-Inventory Problem with Emissions Trading

Sampling Procedure of the Sum of two Binary Markov Process Realizations

THE PREDICTION OF COMPETITIVE ENVIRONMENT IN BUSINESS

Time-interval analysis of β decay. V. Horvat and J. C. Hardy

DEEP UNFOLDING FOR MULTICHANNEL SOURCE SEPARATION SUPPLEMENTARY MATERIAL

Lecture 11 SVM cont

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current :

Robustness Experiments with Two Variance Components

Fuzzy Set Theory in Modeling Uncertainty Data. via Interpolation Rational Bezier Surface Function

Mechanics Physics 151

John Geweke a and Gianni Amisano b a Departments of Economics and Statistics, University of Iowa, USA b European Central Bank, Frankfurt, Germany

Mechanics Physics 151

( t) Outline of program: BGC1: Survival and event history analysis Oslo, March-May Recapitulation. The additive regression model

Dynamic Team Decision Theory. EECS 558 Project Shrutivandana Sharma and David Shuman December 10, 2005

CS286.2 Lecture 14: Quantum de Finetti Theorems II

Variants of Pegasos. December 11, 2009

Lecture 6: Learning for Control (Generalised Linear Regression)

APPROXIMATE ANALYTIC SOLUTIONS OF A NONLINEAR ELASTIC WAVE EQUATIONS WITH THE ANHARMONIC CORRECTION

THE GENERALIZED LAGRANGE'S EQUATIONS OF THE SECOND KIND AND THE FIELD METHOD FOR THEIR INTEGRATION UDC Ivana Kovačić

Scattering at an Interface: Oblique Incidence

Comb Filters. Comb Filters

Optimal environmental charges under imperfect compliance

Pendulum Dynamics. = Ft tangential direction (2) radial direction (1)

On elements with index of the form 2 a 3 b in a parametric family of biquadratic elds

ON THE WEAK LIMITS OF SMOOTH MAPS FOR THE DIRICHLET ENERGY BETWEEN MANIFOLDS

Some Numerical Methods For Solving Fractional Parabolic Partial Differential Equations

Born Oppenheimer Approximation and Beyond

Reactive Methods to Solve the Berth AllocationProblem with Stochastic Arrival and Handling Times

An introduction to Support Vector Machine

Testing a new idea to solve the P = NP problem with mathematical induction

Part II CONTINUOUS TIME STOCHASTIC PROCESSES

CHAPTER 10: LINEAR DISCRIMINATION

Chapter 5. Circuit Theorems

SOME NOISELESS CODING THEOREMS OF INACCURACY MEASURE OF ORDER α AND TYPE β

UNIVERSITAT AUTÒNOMA DE BARCELONA MARCH 2017 EXAMINATION

A Simple Discrete Approximation for the Renewal Function

THE method of moment (MOM) is widely used to extract. Fast Green Function Evaluation for Method of Moment. arxiv: v1 [cs.

Lecture VI Regression

Transcription:

On compung dfferenal ransform of nonlnear non-auonomous funcons and s applcaons Essam. R. El-Zahar, and Abdelhalm Ebad Deparmen of Mahemacs, Faculy of Scences and Humanes, Prnce Saam Bn Abdulazz Unversy, Alhar, 94, KSA. Deparmen of Basc Engneerng Scence, Faculy of Engneerng, Shebn El-Kom, 5, Menofa Unversy, Egyp. Deparmen of Mahemacs, Faculy of Scence, Tabu Unversy, P. O. Box 74, Tabu 749, KSA Absrac: Alhough beng powerful, he dfferenal ransform mehod ye suffers from a drawbac whch s how o compue he dfferenal ransform of nonlnear non-auonomous funcons ha can lm s applcably. In order o overcome hs defec, we nroduce n hs paper a new general formula and s relaed recurrence relaons for compung he dfferenal ransform of any analyc nonlnear non-auonomous funcon wh one or mul-varable. Regardng, he formula n he leraure was found no applcable o deal wh he presen non-auonomous funcons. Accordngly, a generalzaon s presened n hs paper whch reduces o he correspondng formula n he leraure as a specal case. Several es examples for dfferen ypes of nonlnear dfferenal and negro-dfferenal equaons are solved o demonsrae he valdy and applcably of he presen mehod. The obaned resuls declare ha he suggesed approach no only effecve bu also a sragh forward even n solvng dfferenal and negro-dfferenal equaons wh complex nonlneares. Keywords: Dfferenal ransform mehod; Nonlnear non-auonomous funcons; One-dmensonal dfferenal and negro-dfferenal equaons.. Inroducon The Dfferenal Transform Mehod (DTM) whch s based on Taylor seres expanson was frs nroduced by Zhou [] and has been successfully appled o a wde class of nonlnear problems arsng n mahemacal scences and engneerng. The man advanage of he DTM s ha can be appled drecly o nonlnear dfferenal equaons wh no need for lnearzaon, dscrezaon, or perurbaon. Addonally, he DTM does no generae secular erms (nose erms) and does no need o analycal negraons as oher sem-analycal numercal mehods such as HPM, HAM, ADM or VIM and so he DTM s an aracve ool for solvng dfferenal equaons. Alhough hs mehod has been proved o be an effcen ool for handlng nonlnear dfferenal equaons, he nonlnear funcons used n hese sudes are resrced o ceran nds of nonlneares, e.g., polynomals and producs wh dervaves. For oher ypes of nonlnear funcons, Chang and Chang [] consruc a new algorhm based on obanng a dfferenal equaon sasfed by hs nonlnear funcon and hen applyng he DTM o hs obaned dfferenal equaon. Alhough her reamen was found effecve for some forms of nonlneary [,4] sgnfcanly ncreases he compuaonal budge, especally f here are wo or more nonlnear funcons nvolved n he dfferenal equaon beng nvesgaed, as demonsraed by Ebad [5]. Moreover, n he case of complex nonlneares, may be que dffcul o oban he dfferenal equaons sasfed by hese nonlnear funcons. To overcome hs dffculy, a new formula has been derved [5-8] o calculae

he dfferenal ransform of any nonlnear auonomous one varable funcon f ( y ). Ths formula has he same mahemacal srucure as he Adoman polynomals bu wh consans nsead of varable componens. We mean by he nonlnear non-auonomous funcons ha hose nonlnear funcons whch conan he ndependen varable and also he dependen varable and/or s dervaves. Unforunaely, for such ypes of complcaed nonlnear non-auonomous funcons wh one or f, y (), =,,.., m, no relaed formula has been gven o calculae her ransform mul-varable ( ) funcons. Ths provdes he movaon for he presen wor. To overcome he drawbac of he DTM ha s how o compue he dfferenal ransform of hgh complex nonlnear non-auonomous funcons, a generalzed formula s deduced n hs paper for compung he dfferenal ransform of any analyc nonlnear non-auonomous funcon wh one or mul-varable. The proposed mehod deals drecly wh he nonlnear non-auonomous funcon n s form whou any specal nds of ransformaons or algebrac manpulaons. Also, here s no need o compue he dfferenal ransform of oher funcons o oban he requred one. For auonomous funcon, as a specal case of he curren sudy, hese formulas and recurrence relaons have he same mahemacal srucure as he Adoman polynomals bu wh consans nsead of varable componens. The effcency of he proposed mehod s dscussed hrough several es examples ncludng nonlnear dfferenal and negro-dfferenal equaons of dfferen ypes.. Dfferenal Transform Mehod The basc defnons and fundamenal heorems of he one-dmensonal DTM and s applcably for varous nds of dfferenal and negro-dfferenal equaons are gven n [, 9-5]. For convenence of he reader, we presen a bref revew of he DTM n hs secon. The dfferenal ransform of a gven analyc funcon y() n a doman D s defned as d y() Y () =! d =, D, () where y() s he orgnal funcon and Y () s he ransformed funcon. The nverse dfferenal ransform of Y () s defned as. () = y = Y ( ) From Eqs. () and (), we ge d y() y() = ( ) =! d. () = From he above proposon, can be found ha he concep of dfferenal ransform s derved from Taylor seres expanson. In acual applcaons, he funcon y() s expressed by a runcaed seres and Eq. () can be wren as N y = Y ( ), (4) = where N s he approxmaon order of he soluon. Some of he fundamenal mahemacal operaons performed by he one dmensonal dfferenal ransform are lsed n Table.

Table. Some fundamenal operaons of he one dmensonal dfferenal ransform. Orgnal funcon y() Transformed funcon Y () β v() ± w () β V ( ) ±β W ( ) v() w () = V () W ( ) m d v() ( + m)! m V + m d! m! ( β+ ) m Hm [, ] ( β+ )!( m )! λ! e λ λ e m, where Hm [, ] =,, f m f m < v( τ) dτ V ( ), V ( ) u () v() τ dτ G(), = m d v ( q ) ( + m)! m m q + V + m d! ω π sn( ω +β ) sn( ω +β+ )! ω π cos( ω +β ) cos( ω +β+ )!. Dfferenal Transform formulas If a dfferenal equaon conans an analyc nonlnear non-auonomous funcon f (, y() ) hen he dfferenal ransform F( n) of he funcon (, ()) he followng heorems, where we assume ha f (, y() ) f f ( y() ). f y s requred and can be compued from Theorem. The dfferenal ransform F( n) of any analyc nonlnear non-auonomous funcon f (, y() ) a a pon can be compued from he formula n d F( n) = f, Y () n +λ λ (4) dλ = λ= where Y () s he dfferenal ransform of y(). Proof: The dfferenal ransform F n of (, ()) f y s defned as n d F( n) = f (, y() n ) d =. (5) Subsung Eq. n Eq.5 resuls n

n d F( n) = f, Y ( ) n d. (6) = = Now, le =λ, hen Eq.6 becomes n d F( n) = f, Y () n +λ λ. dλ = λ= By hs way, he proof of Theorem s compleed. Theorem. The dfferenal ransform F( n) of any analyc nonlnear non-auonomous funcon f (, y() ) a a pon, sasfes he recurrence relaon where F() f (, Y ()) n F( n) = F( n ) + ( + ) Y F( n ), n =,,.., n = Y () (7) =. Proof: we have f n (, y()) f n (, y() ) f n (, y() ) dy = + y () d (), hen F( n) = f, Y ( ) + f, Y ( ) ( + ) Y ( + ) Y () ( n ) ( n ) = = = = = ( n )! F ( n ) + ( n )! ( + ) Y ( ) F ( n ) = Y () and snce F( n ) s a funcon of and { ()} n Y, hen = n F( n) = F( n ) + ( + ) Y F( n ) n = Y () By hs way, he proof of Theorem s compleed. Thus by Theorems and we have mplemened a new algorhm for compung he one-dmensonal dfferenal ransform of any analyc nonlnear funcon non-auonomous f y. (, ()) We observe ha for auonomous funcon, he defnon (4) and recurrence relaon (7) are reduced o, respecvely n d F( n) = f Y () n λ, (8) dλ = λ= n F( n) = ( + ) Y ( ) F( n ), n =,,... (9) n = Y ( ) One can observe ha he resul n (8) s he presen formula n [5-8] 4

In fac f a sysem of one-dmensonal dfferenal equaons conans a coupled analyc f, y (),,,.., m f, y () f f y () f y ()... f y () nonlneary ( ) =, where we assume ha m m, hen Theorems and can be easly exended usng he above presen procedure o mul-varable funcon and sasfy he followng recurrence algorhms Corollary. The dfferenal ransform F n of any analyc non-auonomous funcon (, ()) f y, =,,.., m a a pon can be defned by n d F( n) = f, Y () n +λ λ dλ, =,,.., m () where Y () s he dfferenal ransform of y (). = λ= Corollary. The dfferenal ransform =,,.., m a a pon, sasfes he recurrence relaon F n of any analyc non-auonomous funcon (, ()) f y, m n F( n) = F( n ) + ( + ) Y ( ) F( n ), n =,,.., n = = Y ( ) () where F() f (, Y ()) =. Moreover for auonomous funcon, he defnon () and recurrence relaon () are reduced, respecvely, o n d F( n) = f Y () n λ, =,,.., m, () dλ = λ= m n F( n) = ( + ) Y ( ) F( n ), =,,.., m, n =,,.., n () = = Y ( ) whch have he same mahemacal srucure as he Adoman polynomals [6] bu wh consans nsead of varable componens. 4. Resuls In hs secon, we have solved dfferen ypes of dfferenal and negro-dfferenal problems wh dfferen forms of nonlnear non-auonomous funcons o demonsrae he valdy and applcably of he presen mehod. Example. Consder he nonlnear nal-value problem y () y() = ln + y(), () y =. (۱٤) Usng he basc properes of DTM and ang he ransform of equaons n (4) resul n 5

( + ) Y ( + ) Y ( ) = F( ), Y () =, =,,,..., (5) where F( ) s he dfferenal ransform of he nonlnear erm ln( + y). F( ) s compued usng he presen mehod and gven by ( Y ), Y () ( + Y () ), Y ( + Y ()) ( )) ( Y )) 4 Y ( Y )) 4( Y ()) + Y () F() = ln( + Y ()), F() = F() = + Y () + () Y () Y () + Y () + Y ( F () = +, + Y () + () + ( Y (4) Y () + Y () Y () + Y () () + Y () F (4) = + + Y () + Y () + Y () + ( + 4 Therefore, a combnaon of (5) and (6) resuls n he seres soluon. (6) 6 4 4 5 y = + + + +.... For suffcenly large number of erms, he closed form of he soluon s y() e =, whch s he exac soluon. Table shows he absolue error obaned for hree varous numbers of erms and a some es pons. Table : Numercal resuls for Example. y y N = 5 N = N = 5..... 9.494e-8 6.e-6 7.9797e-7.4 6.e-6.869e- 4.6e-7.6 7.8e-5 9.565e- 5.55e-7.8 4.6e-4.48e-9.4988e-5..65e-.7e-8 5.8e-4 Example. Consder he nonlnear nal-value problem y () + εy() = εsn( y()), y () =. (7) Tang he dfferenal ransform of equaons n (7) resuls n ( + ) Y ( + ) + ε Y Y ( ) Y ( ) = εf( ), Y () =, =,,,..., (8) = where F( ) s he dfferenal ransform of he nonlnear erm sn( y ( )). F( ) usng he presen mehod and gven by s compued 6

Y () F() =, F() = Y (), F() = Y (), F() = + Y (), 6 5 F(4) = y() Y () y(), F(5) = Y Y () Y () Y () Y + Y (4) Usng (8) and (9), he seres soluon s obaned and gven a ε =. by. (9) 9 47 5 6 45 4 5 6 y = + + +.... The presened resuls are compared wh hose obaned usng MATLAB bul-n solver ode45 n Table. The ode45 solver negraes ODEs usng explc 4h & 5h Runge-Kua (4, 5) formula [7]. In order o guaranee a good numercal reference, ode45 s confgured usng an absolue error of 8 and relave error of. Table : Numercal resuls for Example. y( ) y ( ) N = 5 N = N = 5..... 7.689e-6 8.e- 9.66e-.4 4.55e-4.79e-6.9e-8.6 4.8955e-.5e-4.e-6.8.5675e-.4e-.654e-4. 9.957e-.556e- 8.8e- Example. Consder he followng nonlnear problem wh mulple soluons ( ) y () y() + = +, () y =. () The dfferenal ransform of equaons n () are = + () ( + ) Y ( + ) H(, ) = F( ) ( )! ( + )! and Y () =, where F( ) s he dfferenal ransform of he nonlnear erm + y(). Applyng he presen mehod o he nonlnear funcon f (, y()) = + y() a = and Y () =,resuls n Y () F() =±, F() =±, F() =± +, F() =± Y () + Y () Y () 8 6 4 4 5 F(4) =± Y () + Y () + ( 8 Y () 64 Y ()) Y () + Y (), 8 6 8 8. () 4 Y () Y () Y () 5 Y () Y () Y () 7 Y () F(5) =± + Y (4) + Y () + + Y () Y () 6 8 56 4 where he braces wh posve sgn are due o usng he prncpal square roos whle he braces wh negave sgn are due o usng he negave roos. Therefore, a combnaon of () and () resuls n wo seres soluon gven by 7

y () =±, whch are he exac soluons of (). Example 4. Consder he nonlnear frs order Volerra negro-dfferenal equaon y = cos + + sn ( + y) d τ τ τ, y =, y =. () The dfferenal ransform of equaons n () are π δ( ) F( ) ( + ) Y ( + ) = cos +δ ( ) +, Y () =, Y () =,!, where F( ) s he dfferenal ransform of he nonlnear erm sn ( τ + y ( τ )). By applyng he presen mehod o he nonlnear funcon f ( τ, y( τ)) = sn ( τ + y( τ )) a τ =, Y () = and Y () =, and by usng he prncpal value of he square roo and nverse rgonomerc funcons, we ge F() =, F() =, F() = Y (), F() = Y () +, F(4) = Y (4) + Y (), 6 F(5) Y (5) Y () Y (), F(6) Y () Y (4) Y () Y () Y (6) Y () = + + + = + + + + 4 8 6 5 F(7) 56 Y () 84 Y () Y () Y (4) Y () Y (5) Y (7) Y () = + + + + + + + 8 Hence, he seres soluon s obaned and gven by. () y 6 54 688 5 7 9 = + + + +... For suffcenly large number of erms, he closed form of he soluon s y = sn +, whch s he exac soluon. Table 4 shows he absolue error obaned for hree varous numbers of erms and a some es pons. Table 4: Numercal resuls for Example 4. y( ) y ( ) N = 5 N = N = 5......58e-9 5.55e-6.e-7.4.46e-7.497e- 5.55e-7.6 5.566e-6 9.679e-.e-7.8 4.4e-5.4e-9.e-6..9568e-4.489e-8.7756e-5 Example 5. Consder he nonlnear second order Volerra negro-dfferenal equaon 8

sec τ y () y() y () = + dτ + y ( τ ), y () =, y () =. (4) The dfferenal ransform of equaons n (4) are F( ) ( + )( + ) Y ( + ) = ( + ) Y ( + ) Y ( ) δ( ) +, Y () =, Y () =, Y () =, = sec τ,where F( ) s he dfferenal ransform of he nonlnear erm obaned usng he presen + y ( τ ) mehod a τ = and gven by F() =, F() =, F() =, F() =, F(4) = Y (), Y (5) = Y (4), F(6) = Y (5) + Y () Y (), F(6) = ( Y ()) Y (4) Y (6), 45 7 F(7) 5 Y () Y () Y () Y (5) Y (5) Y (7) Y (4) = + + 5 Hence, he approxmae seres soluon s obaned and gven by (5) 7 6 y 5 5 85 5 7 9 = + + + + +... For suffcenly large number of erms, he closed form of he soluon s y = an, whch s he exac soluon. Table 5 shows he absolue error obaned for hree varous numbers of erms and a some es pons. Table 5: Numercal resuls for Example 5. y( ) y ( ) N = 5 N = N = 5..... 7.8e-7.845e- 8.49e-6.4 9.455e-5.975e-7.89e-.6.7688e-.7649e-5.69e-7.8.58e-.8e-.799e-5. 9.74e-.49e- 9.9e-4 Example 6. Consder he nonlnear Volerra negro-dfferenal equaon wh proporonal delay ( τ ) y sn y = sn + d τ (τ + ) The dfferenal ransform of equaons n (6) are, y () =, y () =. (6) + F π π ( ) ( + ) Y ( + ) = δ( ) sn δ( ) + sn, Y () =, Y () =,,!! = = 9

where F( ) s he dfferenal ransform of he nonlnear erm w τ, w ( τ) = Y ( ) τ (τ + ) obaned usng he presen mehod and gven by = F() =, F() =, F() = 8 Y (), F() = 54 Y () + 54 Y (), F(4) = 8 Y () + 6 Y () 6 Y () + 6 Y (4), F(5) = 486 Y () + (486 Y () 486) Y () 486 Y (4) + 486 Y (5) + 486 Y () Hence, he seres soluon s obaned and gven by. (7) y () = +, whch s he exac soluon. Example 7. Consder he followng nonlnear non-auonomous nal-value ODE sysem y () = y() + + ln y() + y () 4 y () = y () + ln ( + y () ). (8) y() y() =, y () = Applyng he dfferenal ransform o (8), resuls n + + =δ + ( ) Y ( ) ( K ) Y ( ) F( ) ( + ) Y ( + ) = Y ( ) δ ( K) + F ( ). (9) Y () =, Y () = where F( ) and F are he dfferenal ransform of he nonlnear funcons 4 f = ln y and f = ln ( + y ) + y () y(), respecvely. F ( ) and F ( are compued usng formula() and gven by F() =, F() = Y () + + Y (), F() = Y () ( + Y () ) + Y () ( Y () + + Y () ) F() = Y () + ( + Y () ) ( + Y () ) Y () + Y (), ( Y () Y () Y () + Y () )( Y () + + Y () ) + ( Y () + + Y () ) () F() =, F() = Y () Y () F() = Y () Y () Y () + ( + Y () ), F() = Y () + Y () Y () Y () Y () + ( + Y () ) Y () ( + Y () ) 4 () Hence, he seres soluons are obaned and gven as y 6 4 5 = + + +...

y = + + + + + 6 4 4 5... For suffcenly large number of erms, he closed forms of he soluons are () y = e, y () = e, whch are he exac soluons. Table 6 shows he absolue error obaned for hree varous numbers of erms and a some es pons. Table 6: Numercal resuls for Example 7 y y y y N = 5 N = N = 5 N = 5 N = N = 5.........78e-7.e-5.5e-6 9.494e-8 6.66e-6.4e-6.4.759e-5.e- 4.449e-6 6.e-6.87e-.4e-6.6.97e-4.79e-.4e-6 7.8e-5 9.565e- ٤ ٥۱۰۱e-6.8 6.559e-4 4.7e-9.555e-5 4.6e-4.48e-9.9984e-5..455e- 4.69e-8 9.9e-4.65e-.7e-8 5.848e-4 Tables 5 show he absolue errors of he presen mehod for dfferen approxmaon order, N, of he soluon and a some es pons. The resuls show ha he obaned soluons are accurae and converge o he exac ones wh ncreasng he order N. 5. Conclusons In hs paper, a new general formula and hence new recurrence relaons have been derved for compung he dfferenal ransform of any analyc nonlnear non-auonomous funcons wh one or mul-varable. As a specal case of he presen sudy,.e., for auonomous funcon, he curren formulas and recurrence relaons reduces o he same mahemacal srucure as he Adoman polynomals bu wh consans nsead of varable componens n he leraure. I was found ha, he suggesed mehod deals drecly wh he nonlnear non-auonomous funcons, where specal ransformaon or algebrac manpulaons were compleely avoded. In addon, he mehod has been successfully appled on dfferen ypes of dfferenal and nego-dfferenal equaons. Moreover, he obaned seres soluons demonsrae he valdy and applcably of he presen approach. Numercally, he resuls showed ha a fas convergence has been acheved for he obaned seres soluons. An advanage of he presen mehod s ha can be combned wh Padé Approxman (PA), Aferreamen Technques (AT), Power Seres Exender Mehod (PSEM) and mul-sep echnque, among many ohers. Fnally, he auhors beleve ha he presen sudy should be exended o nclude smlar dfferenal and nego-dfferenal equaons n he appled scences, whch ncreases s applcably. Conflcs of Ineres: Auhor has declared ha no compeng neress exs. References. Zhou, J. K., 986. Dfferenal Transformaon and s Applcaons for Elecrcal Crcus, Huazhong Unversy Press, Wuhan Chna 986. Chang, S. H., & Chang, I. L. (8). A new algorhm for calculang one-dmensonal dfferenal ransform of nonlnear funcons. Appled Mahemacs and Compuaon, 95(), 799-88.

. Ebad, A. (). Approxmae perodc soluons for he non-lnear relavsc harmonc oscllaor va dfferenal ransformaon mehod. Communcaons n Nonlnear Scence and Numercal Smulaon, 5(7), 9-97. 4. Ebad, A. (). A relable aferreamen for mprovng he dfferenal ransformaon mehod and s applcaon o nonlnear oscllaors wh fraconal nonlneares. Communcaons n Nonlnear Scence and Numercal Smulaon, 6(), 58-56. 5. Ebad, A. (). On a new dfferenal ransformaon mehod for solvng nonlnear dfferenal equaons. Asan-European Journal of Mahemacs, 6(4), 557. 6. Behry, S. H. (). Dfferenal Transform Mehod for Nonlnear Inal-Value Problems by Adoman Polynomals. Journal of Appled & Compuaonal Mahemacs,. 7. N, H. S., & Soleyman, F. (). A Taylor-ype numercal mehod for solvng nonlnear ordnary dfferenal equaons. Alexandra Engneerng Journal, 5(), 54-55. 8. Faoorehch, H., & Abolghasem, H. (). Improvng he dfferenal ransform mehod: a novel echnque o oban he dfferenal ransforms of nonlneares by he Adoman polynomals. Appled Mahemacal Modellng, 7(8), 68-67. 9. Odba, Z. M. (8). Dfferenal ransform mehod for solvng Volerra negral equaon wh separable ernels. Mahemacal and Compuer Modellng, 48(7), 44-49.. Abdulaw, M. (5). Soluon of Cauchy ype sngular negral equaons of he frs nd by usng dfferenal ransform mehod. Appled Mahemacal Modellng, 9(8), 7-8.. EL-Zahar, E. R. (). Approxmae analycal soluons of sngularly perurbed fourh order boundary value problems usng dfferenal ransform mehod, Journal of Kng Saud Unversy (Scence), 5(), 57 65.. El-Zahar, E. R. (5). Applcaons of Adapve Mul sep Dfferenal Transform Mehod o Sngular Perurbaon Problems Arsng n Scence and Engneerng, Appled Mahemacs and Informaon Scences, 9(), -.. El-Zahar, E. R. (6). Pecewse approxmae analycal soluons of hgh order sngular perurbaon problems wh a dsconnuous source erm, Inernaonal Journal of Dfferenal Equaons, vol. 6, Arcle ID 564, pages, 6. do:.55/6/564. 4. Erür, V. S., Odba, Z. M., & Moman, S. (). The mul-sep dfferenal ransform mehod and s applcaon o deermne he soluons of non-lnear oscllaors. Advances n Appled Mahemacs and Mechancs, 4(4), 4-48. 5. Aroglu, A., & Ozol, I. (8). Soluons of negral and negro-dfferenal equaon sysems by usng dfferenal ransform mehod. Compuers & Mahemacs wh Applcaons, 56(9), 4-47. 6. Duan, J. S. (). Convenen analyc recurrence algorhms for he Adoman polynomals. Appled Mahemacs and Compuaon, 7(), 67-648. 7. Dormand, J. R., & Prnce, P. J. (98). A famly of embedded Runge-Kua formulae. Journal of compuaonal and appled mahemacs, 6(), 9-6.