On The Geometrıc Interpretatıons of The Kleın-Gordon Equatıon And Solution of The Equation by Homotopy Perturbation Method

Similar documents
On Numerical Solutions of Two-Dimensional Boussinesq Equations by Using Adomian Decomposition and He's Homotopy Perturbation Method

Numerical KDV equation by the Adomian decomposition method

New Applications of Adomian Decomposition Method. Emad A. Az-Zo'bi

Approximating Solutions for Ginzburg Landau Equation by HPM and ADM

Comparison between Fourier and Corrected Fourier Series Methods

UNIT 1: ANALYTICAL METHODS FOR ENGINEERS

Mixture of a New Integral Transform and Homotopy Perturbation Method for Solving Nonlinear Partial Differential Equations

Adomian Decomposition Method and its. Modification for Nonlinear. Abel's Integral Equation

The modified Exp-function method and its applications to the generalized K(n,n) and BBM equations with variable coefficients

A Note on Integral Transforms and Differential Equations

The Solution of the One Species Lotka-Volterra Equation Using Variational Iteration Method ABSTRACT INTRODUCTION

Calculus BC 2015 Scoring Guidelines

VARIATIONAL ITERATION METHOD: A COMPUTATIONAL TOOL FOR SOLVING COUPLED SYSTEM OF NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS

Local Fractional Variational Iteration Method for Solving Nonlinear Partial Differential Equations within Local Fractional Operators

REDUCED DIFFERENTIAL TRANSFORM METHOD FOR GENERALIZED KDV EQUATIONS. Yıldıray Keskin and Galip Oturanç

Approximate Solutions for the Coupled Nonlinear. Equations Using the Homotopy Analysis Method

Homotopy Analysis Method for Solving Fractional Sturm-Liouville Problems

Available online at J. Math. Comput. Sci. 4 (2014), No. 4, ISSN:

On the Effective Region of Convergence of the Decomposition Series Solution

STK4080/9080 Survival and event history analysis

6.2 The Moment-Curvature Equations

K3 p K2 p Kp 0 p 2 p 3 p

VIM for Determining Unknown Source Parameter in Parabolic Equations

Research Article The Analytical Solution of Some Fractional Ordinary Differential Equations by the Sumudu Transform Method

Modified Decomposition Method for Solution of Fractional Partial Differential Equations of Two-Sided

SOLVING OF THE FRACTIONAL NON-LINEAR AND LINEAR SCHRÖDINGER EQUATIONS BY HOMOTOPY PERTURBATION METHOD

A TAUBERIAN THEOREM FOR THE WEIGHTED MEAN METHOD OF SUMMABILITY

Section 8. Paraxial Raytracing

S n. = n. Sum of first n terms of an A. P is

Chapter 11 Autocorrelation

ODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003

A Novel Approach for Solving Burger s Equation

Solutions to selected problems from the midterm exam Math 222 Winter 2015

CHAPTER 2. Problem 2.1. Given: m k = k 1. Determine the weight of the table sec (b)

Chapter 9 Autocorrelation

METHOD OF THE EQUIVALENT BOUNDARY CONDITIONS IN THE UNSTEADY PROBLEM FOR ELASTIC DIFFUSION LAYER

Curvilinear Motion: Normal and Tangential Components

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

F D D D D F. smoothed value of the data including Y t the most recent data.

1 Notes on Little s Law (l = λw)

The Moment Approximation of the First Passage Time for the Birth Death Diffusion Process with Immigraton to a Moving Linear Barrier

Electrical Engineering Department Network Lab.

Single Degree of Freedom System Free Vibration

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

Department of Mathematical and Statistical Sciences University of Alberta

APPROXIMATE SOLUTION OF FRACTIONAL DIFFERENTIAL EQUATIONS WITH UNCERTAINTY

Single Degree of Freedom System Free Vibration

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

MODIFIED ADOMIAN DECOMPOSITION METHOD FOR SOLVING RICCATI DIFFERENTIAL EQUATIONS

Parametric Iteration Method for Solving Linear Optimal Control Problems

Review Exercises for Chapter 9

Journal of Applied Science and Agriculture

Samuel Sindayigaya 1, Nyongesa L. Kennedy 2, Adu A.M. Wasike 3

Principles of Communications Lecture 1: Signals and Systems. Chih-Wei Liu 劉志尉 National Chiao Tung University

A Comparative Study of Adomain Decompostion Method and He-Laplace Method

Approximately Quasi Inner Generalized Dynamics on Modules. { } t t R

SUMMATION OF INFINITE SERIES REVISITED

A Complex Neural Network Algorithm for Computing the Largest Real Part Eigenvalue and the corresponding Eigenvector of a Real Matrix

A Comparison Among Homotopy Perturbation Method And The Decomposition Method With The Variational Iteration Method For Dispersive Equation

VISCOSITY APPROXIMATION TO COMMON FIXED POINTS OF kn- LIPSCHITZIAN NONEXPANSIVE MAPPINGS IN BANACH SPACES

ECE-314 Fall 2012 Review Questions

1.225J J (ESD 205) Transportation Flow Systems

Big O Notation for Time Complexity of Algorithms

Dynamic model of large amplitude vibration of a uniform cantilever beam carrying an intermediate lumped mass and rotary inertia

The analysis of the method on the one variable function s limit Ke Wu

Ruled surfaces are one of the most important topics of differential geometry. The

Hadamard matrices from the Multiplication Table of the Finite Fields

Partial Differential Equations

Mean Square Convergent Finite Difference Scheme for Stochastic Parabolic PDEs

Let s express the absorption of radiation by dipoles as a dipole correlation function.

2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

EE757 Numerical Techniques in Electromagnetics Lecture 8

λiv Av = 0 or ( λi Av ) = 0. In order for a vector v to be an eigenvector, it must be in the kernel of λi

University of Mosul. From the SelectedWorks of Mohammed O. Al-Amr

COS 522: Complexity Theory : Boaz Barak Handout 10: Parallel Repetition Lemma

Problems and Solutions for Section 3.2 (3.15 through 3.25)

12 Getting Started With Fourier Analysis

MATH 507a ASSIGNMENT 4 SOLUTIONS FALL 2018 Prof. Alexander. g (x) dx = g(b) g(0) = g(b),

Lecture 15 First Properties of the Brownian Motion

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP)

Application of the Adomian Decomposition Method (ADM) and the SOME BLAISE ABBO (SBA) method to solving the diffusion-reaction equations

Four equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition

CLOSED FORM EVALUATION OF RESTRICTED SUMS CONTAINING SQUARES OF FIBONOMIAL COEFFICIENTS

B. Maddah INDE 504 Simulation 09/02/17

N! AND THE GAMMA FUNCTION

th m m m m central moment : E[( X X) ] ( X X) ( x X) f ( x)

Math-303 Chapter 7 Linear systems of ODE November 16, Chapter 7. Systems of 1 st Order Linear Differential Equations.

Energy Density / Energy Flux / Total Energy in 1D. Key Mathematics: density, flux, and the continuity equation.

Comparison of Adomian Decomposition Method and Taylor Matrix Method in Solving Different Kinds of Partial Differential Equations

MODERN CONTROL SYSTEMS

THE CONSERVATIVE DIFFERENCE SCHEME FOR THE GENERALIZED ROSENAU-KDV EQUATION

Research Article Modified Fractional Variational Iteration Method for Solving the Generalized Time-Space Fractional Schrödinger Equation

Dissipative Relativistic Bohmian Mechanics

A note on deviation inequalities on {0, 1} n. by Julio Bernués*

Extremal graph theory II: K t and K t,t

A Generalized Cost Malmquist Index to the Productivities of Units with Negative Data in DEA

Fuzzy Dynamic Equations on Time Scales under Generalized Delta Derivative via Contractive-like Mapping Principles

Numerical Solution of Parabolic Volterra Integro-Differential Equations via Backward-Euler Scheme

Linear System Theory

Transcription:

Available a hp://pvam.ed/aam Appl. Appl. Mah. SSN: 9-9466 Vol. 7, sse (December ), pp. 69-65 Applicaios ad Applied Mahemaics: A eraioal Joral (AAM) O The Geomerıc erpreaıos of The Kleı-Gordo Eqaıo Ad Solio of The Eqaio by Homoopy Perrbaio Mehod Hasa Bl ad H. Mehme Başkoş Deparme of Mahemaics Fira Uiversiy 9 Elazig, Trkey hbl@fira.ed.r, hmbaskos@gmail.com Received: Je 6, ;Acceped: December 5, Absrac This paper is orgaized i he followig ways: he firs par, we obaied he Klei Gordo Eqaio (KGE) i he Galilea space. he secod par, we applied Homoopy Perrbaio Mehod (HPM) o his differeial eqaio. he hird par, we gave wo eamples for he Klei Gordo eqaio. Fially, We compared he merical resls of his differeial eqaio wih heir eac resls. We also showed ha approach sed is easy ad highly accrae. Keywords: The Galilea space, The Homoopy perrbaio mehod, The Klei-Gordo Eqaio, Liear ad oliear parial differeial eqaios MSC No.: 5A, 5A5, 8Q5. rodcio The Klei-Gordo, Sie-Gordo ad Sih-Gordo Eqaios The relaivisic wave eqaio of he moio of a free paricle wih zero spi fod by physiciss O. Klei ad V. Gordo is called Klei-Gordo eqaio (KGE). f he paricle is characerized by oe space coordiae, ad he he eqaio has he form as 69

6 H. Bl ad H. M. Başkoş m. (.) where is ime,, is wave fcio, ad m is he mass of he paricle. Noe ha Eqaio (.) for m is a classical oe-dimesioal wave eqaio (he eqaio of a vibraig srig) whose solio, has he form f f, where f is a arbirary fcio. By aalogy wih KGE he eqaios si (.) sih (.) are called Sie-Gordo eqaios (SGE) ad Sih-Gordo eqaio (SHGE), respecively. Eqaio (.) has also a impora physical meaig: sice he lef-had side of his eqaio coicides wih he lef-had side of he eqaio of a vibraig srig of he wave [c ad Ugrl (7)] Eqaio (.), i is also a wave eqaio, b, like Eqaio (.), i is oliear (Liao, He (, 4, 6, 7, Bekas e al. (4)) ad describes physical processes relaed o he oliear [Adomia (986)] waves, i pariclar soliary waves (solios) [Drazi(989)] which preserve heir shape der ieracio. This heory is very impora for he heory of plasm. The -dimesioal Galilea ad psedo-galilea spaces ad ca be defied as he affie space E whose hyperplae a ifiiy is edowed by he geomery of he Eclidea space Rosefeld (969) R or he psedo Eclidea space R [see, Rosefeld (969) pp. 95-97]. f a sysem of affie coordiaes i he space E is chose sch ha he basis vecors e, e,, e are direced o he hyperplae a ifiiy of R or R, he disace d bewee X,,, Y y, y,, y is eqal o y. f y, whe wo pois ad d, he hese pois have aoher disace d eqal o he disace bewee he X,,, Y y, y,, y i R or R, respecively. The moios i pois ad ad have he form a, A A a i, j,,,, i i i i i j i where A j is a orhogoal or psedo orhogoal mari, respecively (here he Eisei rle for smmaio is sed). These formlas coicide wih he formlas of rasformaio of orhogoal coordiaes i he -dimesioal isoropic or psedo isoropic spaces or, respecively, is he -dimesioal affie space E whose hyperplae a ifiiy is edowed wih he geomery of he co-eclidea space R * or he copsedo Eclidea space R * correspodig o R ad R i he daliy priciple of he projecive space P. The moios i ad have he from

AAM: er. J., Vol. 7, sse (December ) 6 i, i i i j i A a A a, i, j,,,. i j The hyperplae a ifiiy of R ad plae i he hyperplae -plae, which is he iersecio of all hyperspheres i R or R, form he absoles of ad. For ad he absoles cosis of he plae a ifiiy, lie, ad wo imagiary cojgae or real pois o his lie. Depedig o a posiio relaive o he absole of For ad he lies ad plaes i hese spaces are divided io wo classes: lies of geeral posiio which do o mee he lie, ad special lies which mee he lie: plaes of geeral posiio which do o coai he lie (he plaes or ),ad special plaes which coai his lie (he plaes R or R ). R, ha is, he, ad he absole imagiary or real hyperqadric i his A each poi X i or we deermie orhoormal frames which cosis of vecors e, e, e of legh or i sch ha he lie Xe is a lie of geeral posiio, ad he lies Xe, Xe are special lies which divide harmoically he lies joiig X wih wo imagiary cojgae or real pois of he absole whose eqaios will be wrie as g g, where g g for g g for ad. f a poi X is characerized by a posiio vecor, he he derivaio formlas for hese frames are i e, de e, de e, i d e, de, where i, j,,,,, for eqaios gives ad for. Eerior differeiaio of hese d, d i, i v d, d. v, (.4) where v,. Formlas (.4) show ha he liear forms ad are locally eac differeials, herefore d, dv. (.5) Cosider a crve C of geeral posiio i or. f X is a poi o his crve, e is age vecor o his crve a X, e is a special vecor of he oscillaig plae of his crve a X, ad e is he hird vecor of a orhoormal frame. The derivaio eqaios of his crve are

6 H. Bl ad H. M. Başkoş d d de de de e, ke, e, e, (.6) d d d where is he aral parameer He (), k ad are he crvare ad he orsio of he crve. Cosider a srface S of geeral posiio i or. Le s sppose ha he iersecios of his srfaces wih Eclidea or psedo-eclidea plaes cos. are o sraigh lies, ha is, his srface has o special reciliear geeraors. We deermie a a poi X of his srface he orhoormal frame, whose vecors e ad e are age vecors o S a X ad e is he ormal vecor o S a X, ha is, his vecor is orhogoal o e (he vecors e ad e of his are i a plae = ). The differeial eqaio of Pfaff of he srface S is. (.7) The eerior differeiaio of he eqaio gives, (.8) hece, by meas of he Cara lemma, we obai a b, b c. (.9) The firs fdameal forms of he srface S for geeral crves are ds, (.) ad for special crves are ds g, (.) ha is, iersecios of S, wih plaes. The secod fdameal form of he srface S is d a, e g g a b c. (.) We call a srface i spacelike if g ad imelike if g. The lie of he absole deermies o he srface S, he Koeigs e cosisig of special crves which are iersecios of S wih he plaes, ad of crves of agecy of coes wih apices o he lie of he

AAM: er. J., Vol. 7, sse (December ) 6 absole age o S. The crves of his e are crvare lies of S, sice ormal lies o S alog crves of his e forms developable srface. A he pois of he crvare lies of S of geeral posiio, vecors e of movig frames have cosa direcios, sice hey are direced o he apices of coes, herefore for crvare crves of geeral posiio,. follows from (.5), ha he eqaios of crvare crves of S are cos. v cos. The coordiaes ad v are called caoical coordiaes o he srface S. The pricipal crvares of S, ha is ormal crvares are, respecively, k / for crves ad ac b k c, k g. (.) c Hece, he Gassia crvare K = K e = k k of he srface S is k g ac b K k. (.4) Therefore, he Gassia crvare of a srface S i ad of a imelike srface i is eqal o ac b ad of a spacelike srface i is eqal o b ac. Noe ha he codiio for he srfaces S i ad which have o special reciliear geeraors is he eqaliy c =. The crves o a srface S which are deermied by he eqaio = are asympoic crves. Sice he form is epressed by he formla (.), he codiio for fidig asympoic direcios = / of geeral posiio is a b c. (.5) he case whe vecor e of he movig frame is fied a every poi A o S, he movig frame is caoical ad all oher forms are pricipal, ha is a. (.6) The eerior differeiaio of he forms (.9) ad (.6) ad he sbsiio of epressio (.7), (.6), (.4) ad (.6) io (.4) give - K, (.7) g - a b b ca, (.8) -b c c, (.9)

64 H. Bl ad H. M. Başkoş where he idices p ad p mea Pfaffia derivaives deermied by he formla dp p p. Le he vecor e e be age o a crvare crve of geeral posiio, ha is, he coordiae sysem o he srface S is caoical sysem, v, ad le s fid he correspodig differeial forms of he movig frame. Sice he crvare of a special crvare crve is k dv ds, where v is o agle bewee age lies ad s is he legh of special crve he formlas (.) ad (.) imply ha dv cw. Le s deoe he radis of crvare of his crve by k c (.) he we have dv. (.) By he sbsiio (.) io he secod formla (.6) ad by formlas (.5) ad a, we obai b. (.) Therefore, he formlas (.) have he from k c, k g a. (.) By formlas (.5) ad (.) we ca epress he Pfaffia derivaives p ad p hrogh he parial derivaes p ad p v i he form p p, p cpv. Therefore, by he eqaios (.8), (.9) ad (.) we obai c, av, ha is, a a d dv. v his case formla (.7) ca be wrie as a vv v a. (.4) This formla shows ha he codiios of iegrabiliy of he differeial eqaios of a srface S are redced o sigle differeial eqaio for is pricipal crvares k ad k.

AAM: er. J., Vol. 7, sse (December ) 65 Le a srface S have a crvare K cos = m where. Whe a srface S is referred o he caoical coordiaes, le s show ha he eqaio (.4) ca be redced o he form (.). his case formlas (.) ca be wrie as k c, k Kk m ad also formla (.4) ca be wrie as g m vv m g. (.5) Le s se for a srface i m m, ha is, if we deoe by, vv. ad for a spacelike srface i ; he we obai v / m by, he fcio by for m =, we obai a eqaio. A Aalysis of he HPM A lo of mehods have bee sed o obai solios of parial differeial eqaios i he lierare [He ad Elaga ()]. We cosider HPM which is oe of he mos sed mehods. The firs of all, we ms obai form HMP [Abbasbady (6), He (999)] for HPM. To illsrae he basic ideas of his mehod, we cosider he followig eqaio: f r, r, A (.) wih bodary codiio B,, r, (.) where A is a geeral differeial operaor, B a bodary operaor, f (r) a kow aalyical fcio ad Γ is he bodary of he domai Ω. A ca be divided io wo pars which are L ad N, where L is liear ad N is oliear. Eqaio (.) ca herefore be rewrie as follows; LN f r, r. (.) Homoopy perrbaio srcre is show as followig;

66 H. Bl ad H. M. Başkoş where v p p Lv L p Av f r,, r, p:, (.4) v. (.5) Eqaio (.4), p [, ] is a embeddig parameer ad is he firs approimaio ha saisfies he bodary codiio. We ca assme ha he solio of Eqaio (.4) ca be wrie as a power series i p, as followig; v v pv p v p v (.6), ad he bes approimaio for solio is lim vv v v v, (.7) p The covergece of series Eqaio (.7) has bee proved by He (). This echiqe ca have fll advaage of he radiioal perrbaio echiqes. The series Eqaio (.7) is coverge rae depeds o he o-liear operaor Av ( ) (he followig opiios are sggesed by He (): () The secod derivaive of Nv ( ) wih respec o v ms be small becase he parameer may be relaively largee, i.e., p. () The orm of L ( N / v) ms be smaller ha oe so ha he series coverges.. Applicaios of The HPM Eample. We cosider a liear parial differeial eqaio i order o illsrae he echiqe discssed above. The problem of he form is, (.) where eac solio of he differeial Eqaio (.) is give by; (, ) ( )si (.) ad iiial codiios

AAM: er. J., Vol. 7, sse (December ) 67 (,). Srcre of HPM He (4,,, 9) for Eqaio (.) is p [ Y] p YY Y, '' '', Y py p py py py '', (.) Y p py py (.4) y where Y, Y form as followig; " y ad p,. We sppose ha he solio of Eqaio (.) has he Y Y py p Y p Y p Y, (.5) Y Y py p Y p Y, Y Y py p Y p Y. " " " " " The, sbsiig Eqaio (.5) io Eqaio (.4), ad rearragig based o powers of p - erms, we obai: Y py py py p py py py py py py py py " " " ", " " ", Y py p Y p Y p py p Y p Y py p Y p Y p Y : (.6) " p : Y Y Y (.7) " p : Y Y Y (.8) " p : Y Y Y (.9) wih solvig Eqaio (.6-.9); p Y Y : (,), (.)

68 H. Bl ad H. M. Başkoş " " : p Y Y Y Y Y Y " Y Y Y dd Y, 6 " " : p Y Y Y Y Y Y " Y Y Y dd (.) 5 Y, 5! " " : " p Y Y Y Y Y Y Y Y Y dd (.) 7 Y ( ), 7! he erms of Eqaio (.5) cold easily calclaed. Whe we cosider he series Eqaio (.5) wih he erms Eqaios (.6-.9) ad sppose p, we obai approimaio solio of Eqaio (.) as followig;, Y Y Y Y. (.) As a resl, he compoes Y, Y, Y, Y, are ideified. We obai aalyic solio of Eqaio (.) as followig; 5 7, ( ) 6 54 5 7,! 5! 7!

AAM: er. J., Vol. 7, sse (December ) 69.75.5.5..4.6.8.8.6.4..75.5.5..4.6.8.8.6.4. a. Eac Solio b. Approimaio Solio HPM Figre. The D srfaces for Y i compariso wih he aalyic solio (, ) whe =.5 wih iiial codiio of Eqaio (.) by meas of HPM..9.8.7.6.5 Eac. Sol..4.6.8..9.8.7.6.5. App. Hpm.4.6.8 a. Eac Solio b. Approimaio Solio HPM Figre. The D plos of he merical resls for Y i compariso wih he aalyic solio (, ) whe =.5 wih iiial codiio of Eqaio (.) by meas of HPM Eample. We cosider a oliear parial differeial eqaio give as,,. (.4) The bodary codiios ad iiial codiio are (,) (,) e,, (, ) e, ( ). (.5) Srcre of HPM He (4,,, 9) for Eqaio (.) is

6 H. Bl ad H. M. Başkoş [ ], '' ' p Y p Y Y Y YY '' ', Y py p py py py pyy '' ', (.6) Y p py py pyy (.7) y " y ' y where Y, Y, Y, (.4) has he form as followig; ad p,. We sppose ha he solio of Eqaio Y Y py p Y p Y p Y,, (.8), Y Y py p Y p Y " " " " ", Y Y py p Y p Y (.9) Y Y py p Y p Y ' ' ' ' '. The, sbsiig Eqaio (.9) io Eqaio (.7), ad rearragig based o powers of p - erms, we obai; p Y :, (.) " ' p : Y Y YY Y, (.) " ' ' p : Y Y YY YY Y Y, (.) " ' ' ' p : Y Y YY YY Y YY Y Y, (.) wih solvig Eqaio (.-.); p Y Y Y e : (,) ( ), (.4) " ' " ' p : Y Y YY Y Y Y YY Y, " ' Y Y YY Y d d, " ' Y Y YY Y dd, Y e,!!

AAM: er. J., Vol. 7, sse (December ) 6 " ' ' p : Y Y YY YY Y Y, " ' ' Y Y YY YY Y Y, " ' ' Y Y YY YY Y Y dd, 4 5 Y e, 4! 5! " ' ' ' p : Y Y YY YY Y YY Y Y, " ' ' ' Y Y YY YY Y YY Y Y, " ' ' ' Y Y YY YY Y YY Y Y dd, 6 7 Y e, 6! 7! (.5) (.6) he erms of Eqaio (.8) cold calclaed. Whe we cosider he series Eqaio (.8) wih he erms Eqaio (.4)- Eqaio (.6) ad sppose p, we obai approimaio solio of Eqaio (.4) as followig;, Y Y Y Y (.7) As a resl, he compoes Y, Y, Y, Y, are ideified. We obai aalyic solio of Eqaio (.4) 4 5 6 7, e.!! 4! 5! 6! 7! 5 5..4.6.8..4.6.8.5 5 5 a: Eac Solio b: Approimaio Solio HPM Figre. The D srfaces for Y i compariso wih he aalyic solio (, ) whe =.5 wih iiial codiio of Eqaio (.4) by meas of HPM..4.6.8..4.6.8.5

6 H. Bl ad H. M. Başkoş Table. Absole errors obai for Eample The merical resls for Y i compariso wih he aalyic solio (, ) whe. wih iiial codiio of Eqaio (.) by meas of HPM, ADM, VM. Eac Hpm Eac Vim Eac Adm.,8778E 7 -,96,8778E 7. -5,55E 7 -,6577-5,55E 7. -,98.4,5E 4 -,966,5E 4.5,58E 4 -,6445,58E 4.75.5.5.75.5.5..4.6.8 Eac Sol..75.5.5.75.5.5..4.6.8 Appr. Hpm a. Eac Solio b. Approimaio Solio HPM Figre 4. The D plos for Y i compariso wih he aalyic solio (, ) whe =.5 wih iiial codiio of Eqaio (.4) by meas of HPM Table. Absole errors obai for Eample.. The merical resls for Y i compariso wih he aalyic solio (, ) whe.wih iiial codiio of Eq.(.4) by meas of HPM, ADM, VM. Eac Vim Eac Hpm.,77E 9,6547E 8,77E. 7,768E,484E 6 7,768E.,866E 9,5485E 5,866E 9.4,87949E 8,97E 4,87949E 8.5,E 7,65E 4,E 7 Eac Adm

AAM: er. J., Vol. 7, sse (December ) 6 4. Nmerical Compariso Tables ad show he differece of aalyical solio ad merical solio of he absole error. We also demosrae he merical solio of Eqaio (.) i Figre (a), he correspodig approimae merical solio i Figre (b) ad Eqaio (.4) i Figre (a), he correspodig approimae merical solio i Figre (b). We oe ha oly erms were sed i evalaig he approimae solio. We achieved a very good approimaio wih he acal solio of he eqaios by sig erms oly of he Homoopy perrbaio mehod above. is evide ha he overall errors ca be made smaller by addig ew erms o he perrbaio. Nmerical approimaios shows a high degree of accracy ad i mos cases, he -erm approimaio, is accrae for qie low vales of. The solio is very rapidly coverge by ilizig he homoopy perrbaio mehod. We obaied ha he re of his mehodology jsify from his merical resls, eve i he few erms approimaio is accrae..75.5.5..4.6..8 (a) Eac Solio.8.6.4.75.5.5..4.6.8..6.4 (b) Nmerical Solio (HPM).8.75.5.5..4.6..8 (a) Eac Solio.8.6.4.75.5.5..4.6.8..4.6 (b) Nmerical Solio (ADM).8.75.5.5..4..6..8 (a) Eac Solio.8.6.5.4 8 6 4 Figres A..4.6..8 b) Nmerical Solio (VM).8.6.4

64 H. Bl ad H. M. Başkoş 5 5..4.6.8 (a) Eac Solio.8.6.4. 5 5..4.8.6.4.6..8 (b) Nmerical Solio (HPM) 5 5..4.6.8 (a) Eac Solio.8.6.4. 5 5..4.6.8 (b) Nmerical Solio (ADM)..4.6.8 5 5..4.6.8 (a) Eac Solio.8.6.4. 5 5..4.6.8. (b) Nmerical Solio (VM).4.6.8 Figres B 5. Coclsio The mehod have bee sed for solvig a lo of differeial eqaios sch as ordiary, parial, liear, oliear, homogeeos, ohomogeeos by may researchers. his research, we sed for solvig liear ad oliear Klei-Gordo eqaios wih iiial codiios. Accordig o hese daas sch as D, D graphics ad Tables, oe realize ha oe of he advaages of HPM displays a fas covergece of he solios.

AAM: er. J., Vol. 7, sse (December ) 65 REFERENCES Adomia G. (986). Noliear Sochasic Operaor Eqaios, Academic Press, Sa Diego. Abbasbady S. (6). Applicaio of He s homoopy perrbaio mehod for Laplace rasform, Chaos Solios Fracals,, 6. Bekas, M., Bl, H. ad Erg, M. (4). Geomeric erpreaios of The Klei-Gordo Eqaio ad Solio of The Eqaio By The Adomia Decomposiio Mehod, Fira Uiversiesi Fe ve Mühedislik Bilimler Dergisi, 6(), 4 4. Bl, H. ad Baskos, H.M. (9). A Comparsio Amog Homoopy Perrbaio Mehod Ad The Decomposiio Mehod Wih The Variaioal eraio Mehod For Dispersive Eqaio eraioal Joral of Basic & Applied Scieces JBAS, 9(), 4. Drazi, P. G. ad Johso R.S. (989). Solios: a rodcio, Cambridge Uiversiy Press, New York, USA. He, J.H. (999). Homoopy perrbaio echiqe, Comper Mehods i Applied Mechaics ad Egieerig, 78, 57 6. He, J.H. (6). Some asympoic mehods for srogly oliear eqaios. eraioal Joral of Moder Physics. B, (), 4 99. He, J.H. (4). The homoopy perrbaio mehod for oliear oscillaors wih discoiiies, Applied Mahemaics ad Compaio, 5, 87 9. He, J.H. (). Deermiaio of limi cycles for srogly oliear oscillaors. Physical Review Leer, 9(7), 74-. He, J.H. (). Bookkeepig parameer i perrbaio mehods, eraioal Joral No- Liear Sciece Nmerical Simlaio. (4), 7. He, J.H.(). A coplig mehod a homoopy echiqe ad a perrbaio echiqe for oliear problems, eraioal Joral No-Liear Mechaic, 5, 7 4. He, J.H. ad Elaga S.K. (). A firs corse i fcioal aalysis, Asia Academic Pblisher Limied, Hog Kog. c, M. ad Ugrl, Y. (7). Nmerical Simlaio of he reglarized log wave eqaio by He's homoopy perrbaio mehod, Phys. Le. A 69, 7 79. Liao, S.J. (4). O he homoopy aalysis mehod for oliear problems, Applied Mahemaics ad Comper, 47, 499 5. Rosefeld, B. A. (969). No Eclidea Spaces, Naka, Moscow, RUSSA.