APPLICATION OF CHEBYSHEV APPROXIMATION IN THE PROCESS OF VARIATIONAL ITERATION METHOD FOR SOLVING DIFFERENTIAL- ALGEBRAIC EQUATIONS

Similar documents
Application of He s Variational Iteration Method for Solving Seventh Order Sawada-Kotera Equations

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Haar Wavelet Operational Matrix Method for Solving Fractional Partial Differential Equations

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions

Improved Approximate Solutions for Nonlinear Evolutions Equations in Mathematical Physics Using the Reduced Differential Transform Method

Solving a System of Nonlinear Functional Equations Using Revised New Iterative Method

Fractional Method of Characteristics for Fractional Partial Differential Equations

A NEW TECHNOLOGY FOR SOLVING DIFFUSION AND HEAT EQUATIONS

Variational Iteration Method for Solving Riccati Matrix Differential Equations

Efficient Solution of Fractional Initial Value Problems Using Expanding Perturbation Approach

Application of variational iteration method for solving the nonlinear generalized Ito system

The Application of Optimal Homotopy Asymptotic Method for One-Dimensional Heat and Advection- Diffusion Equations

An Iterative Method for Solving Two Special Cases of Nonlinear PDEs

GENERALIZATION OF THE FORMULA OF FAA DI BRUNO FOR A COMPOSITE FUNCTION WITH A VECTOR ARGUMENT

On the Solutions of First and Second Order Nonlinear Initial Value Problems

Solitons Solutions to Nonlinear Partial Differential Equations by the Tanh Method

Research Article Convergence of Variational Iteration Method for Second-Order Delay Differential Equations

Iterative Laplace Transform Method for Solving Fractional Heat and Wave- Like Equations

Chapter 2. First Order Scalar Equations

An Efficient Technique in Finding the Exact Solutions for Cauchy Problems

Numerical Dispersion

Solution of Integro-Differential Equations by Using ELzaki Transform

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

An Invariance for (2+1)-Extension of Burgers Equation and Formulae to Obtain Solutions of KP Equation

Chapter 4. Truncation Errors

Positive continuous solution of a quadratic integral equation of fractional orders

Modified Iterative Method For the Solution of Fredholm Integral Equations of the Second Kind via Matrices

Ordinary Differential Equations

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)

Sumudu Decomposition Method for Solving Fractional Delay Differential Equations

Research Article Solving the Fractional Rosenau-Hyman Equation via Variational Iteration Method and Homotopy Perturbation Method

New Seven-Step Numerical Method for Direct Solution of Fourth Order Ordinary Differential Equations

LAPLACE TRANSFORM AND TRANSFER FUNCTION

Undetermined coefficients for local fractional differential equations

Research Article Multivariate Padé Approximation for Solving Nonlinear Partial Differential Equations of Fractional Order

Exact travelling wave solutions for some important nonlinear physical models

Method For Solving Fuzzy Integro-Differential Equation By Using Fuzzy Laplace Transformation

Available online Journal of Scientific and Engineering Research, 2017, 4(10): Research Article

ENGI 9420 Engineering Analysis Assignment 2 Solutions

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

Time-fractional Klein-Gordon equation: formulation and solution using variational methods

International Journal of Emerging Technologies in Computational and Applied Sciences (IJETCAS)

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

CONTRIBUTION TO IMPULSIVE EQUATIONS

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

Differential Equations

The expectation value of the field operator.

6.2 Transforms of Derivatives and Integrals.

AN APPROXIMATION SOLUTION OF THE 3-D HEAT LIKE EQUATION

A New Perturbative Approach in Nonlinear Singularity Analysis

Exact travelling wave solutions for some important nonlinear physical models

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

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

Multi-scale 2D acoustic full waveform inversion with high frequency impulsive source

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations

THE SOLUTION OF COUPLED MODIFIED KDV SYSTEM BY THE HOMOTOPY ANALYSIS METHOD

A novel solution for fractional chaotic Chen system

THE FOURIER-YANG INTEGRAL TRANSFORM FOR SOLVING THE 1-D HEAT DIFFUSION EQUATION. Jian-Guo ZHANG a,b *

Chapter 3 Boundary Value Problem

Symmetry and Numerical Solutions for Systems of Non-linear Reaction Diffusion Equations

Solutions for homework 12

Vanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law

Research Article A Coiflets-Based Wavelet Laplace Method for Solving the Riccati Differential Equations

Algorithm Analysis of Numerical Solutions to the Heat Equation

A residual power series technique for solving systems of initial value problems

Exact solution of the(2+1)-dimensional hyperbolic nonlinear Schrödinger equation by Adomian decomposition method

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

Average Number of Lattice Points in a Disk

Math 23 Spring Differential Equations. Final Exam Due Date: Tuesday, June 6, 5pm

System of Linear Differential Equations

Legendre wavelet collocation method for the numerical solution of singular initial value problems

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du.

The Contradiction within Equations of Motion with Constant Acceleration

Robust estimation based on the first- and third-moment restrictions of the power transformation model

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

Mathematical Theory and Modeling ISSN (Paper) ISSN (Online) Vol.2, No.4, 2012

Solutions to Assignment 1

Department of Mechanical Engineering, Salmas Branch, Islamic Azad University, Salmas, Iran

Stability and Bifurcation in a Neural Network Model with Two Delays

10. State Space Methods

Recursive Least-Squares Fixed-Interval Smoother Using Covariance Information based on Innovation Approach in Linear Continuous Stochastic Systems

After the completion of this section the student. Theory of Linear Systems of ODEs. Autonomous Systems. Review Questions and Exercises

Research Article An Unconventional Finite Difference Scheme for Modified Korteweg-de Vries Equation

arxiv: v1 [math.fa] 3 Jan 2019

The Optimal Stopping Time for Selling an Asset When It Is Uncertain Whether the Price Process Is Increasing or Decreasing When the Horizon Is Infinite

D Alembert s solution of fractional wave equations using complex fractional transformation

International Journal of Mathematics Trends and Technology (IJMTT) Volume 37 Number 3 September 2016

Class Meeting # 10: Introduction to the Wave Equation

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

-e x ( 0!x+1! ) -e x 0!x 2 +1!x+2! e t dt, the following expressions hold. t

Online Appendix to Solution Methods for Models with Rare Disasters

Short Introduction to Fractional Calculus

Inventory Control of Perishable Items in a Two-Echelon Supply Chain

The fundamental mass balance equation is ( 1 ) where: I = inputs P = production O = outputs L = losses A = accumulation

15. Vector Valued Functions

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

Numerical Solution of Fractional Variational Problems Using Direct Haar Wavelet Method

AN EFFICIENT METHOD FOR SOLVING FRACTIONAL DIFFERENTIAL EQUATIONS USING BERNSTEIN POLYNOMIALS

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

Transcription:

Mahemaical and Compuaional Applicaions, Vol., No. 4, pp. 99-978,. Associaion for Scienific Research APPLICATION OF CHEBYSHEV APPROXIMATION IN THE PROCESS OF VARIATIONAL ITERATION METHOD FOR SOLVING DIFFERENTIAL- ALGEBRAIC EQUATIONS M. Ghovamand, M.M. Hosseini, M. Nilli Faculy of Mahemaics, Yazd Universiy, P.O. Bo 8995-74,Yazd, Iran. mghova@su.yazduni.ac.ir, hosse_m@yazduni.ac.ir Absrac- In his paper, we use Chebyshev approimaions in he process of He s variaional ieraion mehod for finding he soluion of differenial-algebraic equaions. This allows us o make inegraion a each of he ieraions possible and a he same ime, obain a good accuracy in a reasonable number of ieraions. Numerical resuls show ha using Chebyshev approimaion is much more efficien han using Taylor approimaion which is more popular. Firs, an inde reducion echnique is implemened for semi-eplici differenialalgebraic equaions, hen he obained problem is solved by He s variaional ieraion mehod. The scheme is esed for some high inde differenial-algebraic equaions and he resuls demonsrae reliabiliy and efficiency of he proposed mehod. Key words- Chebyshev approimaion, Variaional ieraion mehod, Differenial algebraic equaions. INTRODUCTION Many physical problems are governed by a sysem of differenial-algebraic equaions (DAEs), and finding he soluion of hese equaions has been he subjec of many invesigaions in recen years. In 999, he variaional ieraion mehod (VIM) was proposed by He [-]. This mehod is now widely used by many researchers o sudy linear and nonlinear problems. The mehod inroduces a reliable and efficien process for a wide variey of scienific and engineering applicaions. I is based on Lagrange muliplier and i has he meris of simpliciy and easy eecuion. Unlike he radiional numerical mehods, VIM needs no discreizaion, linearizaion, ransformaion or perurbaion. The mehod gives rapidly convergen successive approimaions of he eac soluion if such a soluion eiss; oherwise a few approimaions can be used for numerical purposes. The VIM was successfully applied o auonomous ordinary and parial differenial equaions [ 4]. Recenly in [5] he VIM has been implemened for finding he soluion of differenialalgebraic equaions. To avoid edious inegraion, in he laer paper he Taylor approimaion is used. In his paper, we are going o use he Chebyshev approimaion insead of Taylor approimaion. Eamples show ha his procedure is much more efficien. I is well known ha he eigenfuncions of cerain singular Surm-Liouville problems allow he approimaion of funcions [a, b] where runcaion error approaches zero faser han any negaive power of he number of basic funcions used in he approimaion, as ha number (order of runcaion ) ends o infiniy []. This phenomenon is usually referred o as '' specral accuracy ''. In his work, we are using C

97 M. Ghovamand, M.M. Hosseini and M. Nilli firs kind orhogonal Chebyshev polynomials T k k which are eigenfuncions of singular Surm-Liouville problem: k T () Tk (). DAEs AND REDUCING INDEX I is well known ha he inde of DAEs is a measure of he degree of singulariy of he sysem and also widely regarded as an indicaion of cerain difficulies for numerical mehods. So, DAEs can be difficul o solve when hey have a higher inde, i.e., an inde greaer han [7]. In his case, an alernaive reamen is he use of inde reducion mehods [7-9]. In his secion, we briefly review he reducing inde mehod for DAEs which is menioned in [8]. Consider he linear (or linearized) semi-eplici DAEs: X (m) m A X BY q, (a) j j ( j) CX r, (b) where A, B and C are smooh funcions of, j nk kn f, A j nn () R, j,, m, B() R, C() R, n, k n and CB is nonsingular (DAE has inde m ) ecep possibly a a finie number of isolaed poins of. The n inhomogeniies are q() R and r() R. Now suppose ha CBis non-singular, from (a), we can wrie m (m) ( j) Y (CB) CX A jx q, j [, f ] () Subsiuing () ino (a) implies ha m ( m) ( j) I B( CB) CX A j X q j So, problem () ransforms o he over-deermined sysem: m ( m) ( j) I B( CB) C X A j X q, j () CX r, [, f ] Now sysem () can be ransformed o a full-rank DAE sysem wih n equaions and n unknowns wih inde m [8]. Here, for simpliciy, we consider problem () when m (problem has inde ). Theorem : Consider problem () wih inde, n and k. This problem is equivalen o he following inde -DAE sysem:

Applicaion of Chebyshev Approimaion 97 EX EX qˆ (4) such ha ba b a ba b a b b b q bq E, E, c c qˆ r and y (CB) C[X AX q]. (5) Proof: presened in [8]. In his paper, firs we implemen his proposed inde reducion mehod o linear semieplici DAEs. Then we employ he VIM using Chebyshev approimaion o solve he obained problem. Furhermore, we use some eamples o demonsrae he efficiency and effeciveness of he proposed mehod.. HE S VARIATIONAL ITERATION METHOD In his secion, we briefly review he main poins of he powerful mehod, known as he He s variaional ieraion mehod. This mehod is a modificaion of a general Lagrange muliplier mehod proposed by Inokui []. In he VIM, he differenial equaion L[u()] N[u()] g(), () is considered, where L and N are linear and nonlinear operaors, respecively, and g() is an inhomogenous erm. Using he mehod, he correcion funcional u N[u ~ n () u n () [L(u n (s)) n (s)] g(s)]ds (7) is considered, where is a general Lagrange muliplier, is he n -h approimae soluion and u~ n is a resriced variaion which means u~ n. In his mehod, firs we deermine he Lagrange muliplier ha can be idenified via variaional heory, i.e., he muliplier should chosen such ha he correcion funcional is saionary, i.e., u~ n (u n (), ). Then he successive approimaion u n, n of he soluion u will be obained by using any selecive iniial funcion u and he calculaed Lagrange muliplier. Consequenly, u lim u. I means ha, by he correcion n funcional (7) several approimaions will be obained and herefore, he eac soluion emerges as he limi of he resuling successive approimaions. To perform he VIM, in general, for an arbirary naural number, g () epress in Taylor series, g () gi (). (8) i In his paper, we sugges ha g () be epressed in Chebyshev series, n u n

97 M. Ghovamand, M.M. Hosseini and M. Nilli i g() a T (), (9) i i where T i () is he firs kind of orhogonal Chebyshev polynomial, T (), () T, T (), and in general, Tk Tk Tk, k. In he ne secion, his mehod is successfully applied for solving differenial-algebraic equaions. 4. TEST PROBLEMS In his secion, o show he abiliy and efficiency of he proposed mehod, some eamples are presened. In all he eamples, o simplify he compuaions, for an arbirary naural number, every coefficien funcion g() is epressed in Chebyshev series (9). The resuls are compared wih he case in which Taylor epansion is used wih he same number of erms. The algorihms are performed by Maple wih digis precision. Eample : Consider inde- problem: X AX By q, (a) CX r, (b) where and sin() A, B, q, C T, r() (e sin()), wih (), () and he eac soluions () e, () sin() and cos() y(). From Theorem, problem () can be convered o he inde- DAE: e sin() (a) () sin() (b) wih (), and (). To solve he new problem, we ransform he algebraic equaion (a) in he ieraive form wih respec o and by he He s variaional ieraion mehod and using (7), we consruc he correcion funcional in -direcion for he differenial equaion (b). Therefore, we obain he following (n) syse () e sin() () (a) () (n ) () () (s)[ (s) (s) ~ (s) sin(s)]ds (b)

Applicaion of Chebyshev Approimaion 97 where ~ is considered as a resriced variaion,i.e., ~. By aking he variaion from boh sides of he correcion funcional (b), we have (n) ~ () ~ (s)[ (s) (s) ~ (s) sin(s)]ds, or (n) ~ () ~ (s) (s) s [ (s) (s)] (s)ds. (n) By imposing ~, we obain he saionary condiions (s) s (s) (s). Therefore s (s) e. (4) By subsiuing he opimal value (4) ino funcional (b), we obain he following ieraion formula: (n) (n) e sin() e s [ () (s) () (s) ~ () (s) sin(s)]ds, wih n,,,, () and (). Now, we epand he coefficien funcions e and sin() a and e a Taylor series epansion wih v as follow: e 4 4 5 7 9 54 7 4 8 (a) (b) s 88 s by 9, () (5) (a) sin(), (b) e s 5 7 54 88 ( s) ( s) s 7 ( s) 9 54 So afer ieraions, (5) and () yield: 4 ( s) ( s) 7 4 4 ( s) ( s) 8 5 88 ( s) 9 (c). () () () () () () () () 4 4 4 5 7 54 4 4 88 5 9 88 99584 88 99584 In he alernaive mehod, we epanded he coefficien funcions e, sin() and Chebyshev series wih he same number of erms. Using (5) and (), afer ieraions, we obain s e by

974 M. Ghovamand, M.M. Hosseini and M. Nilli () () () () ().79( 4) 4.( ).7( 8) ().. 7.8 ( ) ().79( 4)..( 5) ()...4( 5) 9 9 For he sake of comparison, we have illusraed he absolue errors for () () and using boh Taylor and Chebyshev cases in figures and. These figures, obviously, show he superioriy of using Chebyshev approimaion insead of Taylor approimaion in his eample. I should be noed ha in order o increase he rae of convergence, we have used (n ) insead of in (5b) for compuing (n ). Fig.. Absolue errors of using Taylor polynomials for compuaion of (n) and... in E.. (n )

Applicaion of Chebyshev Approimaion 975 Fig.. Absolue errors of using Chebyshev polynomials for compuaion of (n ) (n) and... in E.. Eample : Consider inde- problem: X AX By q, (7a) CX r, (7b) where and A, C T e ( sin() ) B, q sin(), e (sin() cos() ) r() e ( sin()) wih () () and he eac soluions () e, () e sin() e and y(). By Theorem, he inde - DAEs (7) ransforms o he following inde- DAEs: g() (a) (8) g () g(), (b) wih () (), when g() e ( sin(), g () and g() e (cos() sin()). Similar o eample, we ransform he algebraic equaion (8a) in he ieraive form wih respec o and consruc he suiable correcion funcional in -direcion by using (7) for he differenial equaion (8a). Therefore, sysem (8) is epressed as

97 M. Ghovamand, M.M. Hosseini and M. Nilli (n) () g() (a) (n) s ~ (s) s ~ (s) g (s) ~ (9) () (s) (s) (s) g(s) ds, (b) where ~ and ~ denoe resriced variaions, i.e., ~ ~.To find he opimal value of in (9b), we have (n) () () (s) (s) s ~ (s) s ~ (s) g (s) ~ (s) g (s) ds. Therefore (n) () () (s) (s) s (s) (s)ds. (n) Imposing ~ yields he following saionary condiions: (s) s () (s). Therefore he opimal value of Lagrange muliplier is ( s). () By subsiuing his value ino correcion funcional (9b), he following ieraion formula is obained: (n) () g() (a ) (n) () (s) s ~ (s) s ~ (s) g (s) ~ () (s) g(s) ds (b) () wih n,,,..., () and (). We epand he funcions g (), g () and g () by Taylor series epansion a wih v 4.So afer 8 ieraions, () yields () () (8) (8) () () () () 4 4 5 4 5 () 884 884 5 4 799877 8858 799877 5 8858...... In he alernaive mehod, we epanded he coefficien funcions e, sin( ) and by Chebyshev series wih he same number of erms. Using (7) and (8), afer 8 ieraions, we obain () 4 ().74( 8)..8( 8) () () 9.99( ) 5.( ).97( 9) (8) 9 ().74( 8)..( 4) (8) 9 () 9.99( )..44( )... s e

Applicaion of Chebyshev Approimaion 977 For he sake of comparison, we have illusraed he absolue errors for (8) (8) and using boh Taylor and Chebyshev cases in able. This Table, obviously, shows he superioriy of using Chebyshev approimaion insead of Taylor (n ) approimaion in his eample. In his eample, we have used insead of in (b) o compue (n ). Absolue errors of using Taylor polynomials for compuaion of ~ and ~ in E.. ~ () () ~ () ()..5( 8).5( 7)..9( ).57( )..4( ).7( ).4.55( 8).88( 8).5 5.9( 7).8( ) Table ) ) 9 ) 4 ) ) ) The comparison beween he resuls menioned in Figures and and Table show he power of he proposed mehod of his paper, for hese eamples. 5. CONCLUSION Absolue errors of using Chebyshev polynomials for compuaion of ~ and ~ in E.. ~ () ( ~ () ().8( 5.8( 4).5( 4.79( 4).9( 4 9.7( 4) 4.( 4.8( 4).79( 4.57( ) The variaional ieraion mehod (VIM) has been successful for solving many applicaion problems. However, difficulies may arise in dealing wih deermining he componens u m, (7). To overcome hese difficulies he modified VIM is proposed using Chebyshev polynomials and is applied for solving differenial algebraic equaions in his paper. The resuls are compared wih he VIM using Taylor series. Numerical resuls show ha using Chebyshev approimaion is much more efficien han using Taylor approimaion which is more popular. The proposed mehod can be easily generalized for more funcional equaions.. REFERENCES [] J. H. He, Variaional ieraion mehod- a kind of non-linear analyical echnique: Some eamples, Inernaional Journal of Nonlinear Mechanics 4 99 78, 999. [] J. H. He, Variaional ieraion mehod for auonomous ordinary differenial sysems, Applied Mahemaics and Compuaion 4 5,. [] J. H. He, Variaional ieraion mehod _ some recen resuls and new inerpreaions, Journal of Compuaional and Applied Mahemaics 7-7, 7. [4] T. A. Abassy, Modified variaional ieraion mehod (nonlinear homogeneous iniial value problem), Compuers & Mahemaics wih Applicaions 59 9-98,.

978 M. Ghovamand, M.M. Hosseini and M. Nilli [5] S. Abbasbandy and E. Shivanian, Applicaion of he variaional ieraion mehod for sysem of nonlinear Volera s inegro-differenial equaions, Mahemaical and Compuaional Applicaions 4 47-58, 9. [] F. Geng and Y. Lin, Applicaion of he variaional ieraion mehod o inverse hea source problems, Compuers & Mahemaics wih Applicaions 58 98-, 9. [7] J. H. He and X. H. Wu, Variaional ieraion mehod: New developmen and applicaions, Compuers & Mahemaics wih Applicaions 54 88-894, 7. [8] J. H. He and X. H. Wu, Variaional ieraion mehod for Surm Liouville differenial equaions, Compuers & Mahemaics wih Applicaions 58-8, 9. [9] A. A. Hemeda, Variaional ieraion mehod for solving wave equaion, Compuers & Mahemaics wih Applicaions 5 948-95, 8. [] S. Momeni, S. Abuasad and Z. Odiba, Variaional ieraion mehod for solving nonlinear boundary value problems, Applied Mahemaics and Compuaion 8 5-58,. [] Z. Odiba and S. Momani, The variaional ieraion mehod: An efficien scheme for handling fracional parial differenial equaions in fluid mechanics, Compuers & Mahemaics wih Applicaions 58 99-8, 9. [] J. Saberi-Nadjafi and M. Tamamgar, The variaional ieraion mehod: A highly promising mehod for solving he sysem of inegro-differenial equaions, Compuers & Mahemaics wih Applicaions, 5 4-5, 8. [] M. Taari and M. Dehghan, Improvemen of He s variaional ieraion mehod for solving sysems of differenial equaions, Compuers & Mahemaics wih Applicaions 58 -, 9. [4] A. M. Wazwaz, The variaional ieraion mehod for eac soluion of Laplace equaion, Physics Leers A -, 7. [5] F. Solanian, S. M. Karbassi and M. M. Hosseini, Applicaion of He s variaional ieraion mehod for soluion of differenial-algebraic equaions, Chaos, Solions and Fracals 4 4-445, 9. [] C. Canuo, M. Y. Hussaini, A. Quareroni and A. Zang, Specral mehods in fluid dynamics, Springer-Verlag, 998. [7] H. Wang and Y. Song, Regularizaion mehods for solving differenial-algebraic equaions, Applied Mahemaics and Compuaion 9 8 9,. [8] E. Babolian and M. M. Hosseini, Reducing inde, and specral mehod for differenial-algebraic equaions, Applied Mahemaics and Compuaion 4 77-9,. [9] M. M. Hosseini, An inde reducion mehod for linear Hessenberg sysems, Applied Mahemaics and Compuaion 7 59-, 5. [] M. Inokui, H. Sekine and T. Mura, General use of he Lagrange mulipliers in nonlinear mahemaical physics. In: Nema-Nasser S, edior. Variaional mehod in he mechanics of solids. Oford: Pergamon Press; 978. p.5-.