Solving the systems of operator equations by iterative methods

Abstract

Let \(X,Y\) be two Banach spaces and \(Z=X\times Y\). We consider the system of nonlinear equations \[x=\varphi \left( x,y\right),\\ y=\psi \left(x,y\right),\] where \(\varphi:Z\rightarrow X\), \(\psi:Z\rightarrow Y\). Assuming that \(\varphi\) and \(\psi \ \) satisfy Lipschitz conditions we study the convergence of the Gauss-Seidel type method \[x_{n}=\varphi \left(x_{n-1},y_{n-1}\right), \\ y_{n}=\psi \left( x_{n},y_{n-1}\right) .\] The obtained result is applied to the solving of a linear system, for which the matrix is splitted in four submatrices. We illustrate the obtained results for some numerical examples.

Authors

Ion Păvăloiu
(Tiberiu Popoviciu Institute of Numerical Analysis)

Title

Original title (in French)

La résolution des systèmes d’équations opérationnelles à l’aide des méthodes itératives

English translation of the title

Solving the systems of operator equations by iterative methods

Keywords

Gauss-Seidel method, system of equations in Banach spaces, linear systems

Cite this paper as:

I. Păvăloiu, La résolution des systèmes d’équations opérationnelles à l’aide des méthodes itératives, Mathematica, 11(34) (1969), pp. 137-141 (in French).

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PDF-Latex version of the paper. (English translation)

About this paper

Journal

Mathematica

Publisher Name

Academia R.S. Romania

DOI

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Solving the systems of operator equations by iterative methods

by
Ion Păvăloiu
in Cluj

1. LetXAndANDtwo Banach-type spaces andWITH=X×ANDthe Cartesian product of these spaces.

In spaceWITHwe will consider the following equation:

(1) x =f⁢(x,and)
and =ψ⁢(x,and).

In this note we will interpret the previous equation as a system of two equations with two unknowns where fAndψare operators defined onWITHand values ​​respectivelyXAndAND.In this way, we will highlight a convergence criterion of the Gauss-Seidel process applied to the resolution of this system. Then we will show that this criterion is more general than those that are known.

Finally, the results obtained will be applied to the development of a new method for solving systems of linear equations.

Part of the results of this note were obtained by us in a particular case(X=AND=ℝ)in work [ 2 ] .

2. We assume that the operatorsfAndψsatisfy the following conditions:

a) OperatorsfAndψtransform the field D⊂WITHin himself.

b) There are constantsa,b,has andbsuch as

‖ψ⁢(x2,and2)−ψ⁢(x1,and1)‖ ≤a⁢‖x2−x1‖+b⁢‖and2−and1‖
‖f⁢(x2,and2)−f⁢(x1,and1)‖ ≤a⁢‖x2−x1‖+b⁢‖and2−and1‖

for everything(xi,andi)∈D,i=1,2.

Theorem 1 .

If the operatorsfAndψsatisfy conditions a) and b), where the constantsa,b, aAndb satisfy the inequalities:

(2) a+b+a⁢b <2,
(1−a)⁢(1−b) >a⁢b,

then we have the following properties:

a') The system ( 1 ) has only one solution(x¯,and¯)∈D¯

b') The iterative process

(3) xn =f⁢(xn−1,andn−1),
andn =ψ⁢(xn,andn−1),n=1,2,…,(x0,and0)∈D

is convergent and we have:

x¯ =limn→∞xn,and¯=limn→∞andn.
Demonstration.

We will first show that we have property b'). To do this we will observe that the partial sums of the following two series

(4) x0+∑i=1∞(xi−xi−1)
and0+∑i=1∞(andi−andi−1)

coincide with the terms of the sequence ( 3 ). Noting

fn−1 =‖xn−xn−1‖,
gn−1 =‖andn−andn−1‖,n=1,2,…,

and taking into account conditions b) we obtain the following inequalities

fn ≤a⁢fn−1+b⁢gn−1
gn ≤a⁢fn+b⁢gn−1,n=1,2,….

Now using Lemma 2 [ 2 ] it follows that if conditions ( 2 ) hold then there exists a constantC independent ofnsuch that we have

fn ≤C⁢h1n−1⁢k1n−1,
gn ≤C⁢h1n⁢k1n−1

and that the series∑i=0∞fi,∑i=0∞giare convergent, where0≤h1⁢k1<1,(h1,k1)being a positive solution of the following algebraic system:

a+b⁢h =k⁢h
a⁢k+b =k⁢h.

This results in the absolute convergence of the series ( 4 ) and therefore the convergence of the process ( 3 ). Ifx¯And and¯are the limits of the sequences ( 3 ) then taking into account b) it results that(x¯,and¯)is a solution for the system ( 1 ).

For uniqueness we will assume that the system ( 1 ) has two solutions(x¯,and¯)∈D¯And (x¯1,and¯1)∈D¯so we have

‖x¯−x¯1‖ ≤a⁢‖x¯−x¯1‖+b⁢‖and¯−and¯1‖
‖and¯−and¯1‖ ≤a⁢‖x¯−x¯1‖+b⁢‖and¯−and¯1‖

from which we deduce

‖x¯−x¯1‖ ≤b⁢a(1−b)⁢(1−a)⋅‖x¯−x¯1‖
‖and¯−and¯1‖ ≤b⁢a(1−b)⁢(1−a)⋅‖and¯−and¯1‖

which contradicts the fact that(1−b)⁢(1−a)>a⁢b. ∎

Noticed .

Anda,b,aAndbmeet the conditions a+b<1,a+b<1ora+a<1,b+b<1then conditions ( 2 ) are verified.

The error evaluation is given by the following inequalities:

‖x¯−xn‖ ≤C⁢h1n−1⁢k1n−11−h1⁢k1
‖and¯−andn‖ ≤C⁢h1n⁢k1n−11−h1⁢k1,n=1,2,….\alignqed

3. The results presented previously will be applied to the resolution of systems of linear equations of the form

(5) X=A⁢X+b

OrX∈ℝnis the unknown,A=(ai,j);i,j=1,n¯is the system matrix andb∈ℝn is the free term.

To resolve the system ( 5 ) we will decompose the matrixAin the matricesM1,M2,M3,M4of the following types.M1is a matrix of the type(s,s),M2is of the type(s,n−s),M4is of the type(n−s,s)AndM4is of the type(n−s,n−s), 1≤s<n, that is to say thatAhas the following form

A=(M1⋮M2⋯⋯M3⋮M4)𝑠⁢s.

It should also be noted

X=(inin)⁢And ⁢b=(b1b2)

Orin,b1∈ℝsAndin,b2∈ℝn−s.Thus the system ( 5 ) can be written in the form:

(6) in =M1⁢in+M2⁢in+b1
in =M3⁢in+M4⁢in+b2

OrinAndinare the vectors of the unknowns,(in,in)∈ℝs×ℝn−s.

To resolve the system ( 6 ) we will apply the following iterative process:

(7) ini =M1⁢ini−1+M2⁢ini−1+b1
ini =M3⁢ini+M4⁢ini−1+b2,i=1,2,…,(in0,in0)∈ℝs×ℝn−s.

This iterative process results as an application of the process ( 3 ) exposed in the first part of this note.

Applying Theorem 1 we will obtain the

Theorem 2 .

If the matricesM1,M2,M3AndM4satisfy the following inequalities:

(8) ‖M1‖+‖M4‖+‖M2‖⁢‖M3‖ <2
(1−‖M1‖)⁢(1−‖M4‖) >‖M3‖⁢‖M2‖

then the system ( 6 ) has only one solution(in¯,in¯)∈ℝs×ℝn−sand the method ( 7 ) converges to this solution.

We have thus obtained a new iterative method for solving systems of equations. This method converges under much more general conditions than the simple iteration method or the Gauss-Seidel method. This fact will be illustrated by the following numerical example.

4. Given the system:

(9) x1 =0.02⁢x1+0.045⁢x2+8⁢x3+0.4
x2 =0.05⁢x1+0.042⁢x2+3⁢x3−0.6
x3 =0.003⁢x1+0.013⁢x2+0.45⁢x3−0.8.

It should be noted

in =(x1x2),in=(x3),
M1 =(0.02 0.0450.05 0.042),M2=(83)
M3 =(0.003, 0.013),M4=(0.45),
b1 =( 0.4−0.6),b2=(−0.8).

If we consider the uniform norm for these matrices we have

‖M1‖ =0.092,
‖M2‖ =8,
‖M3‖ =0.016⁢And
‖M4‖ =0.45.

We will check whether with these values ​​the conditions ( 8 ) are fulfilled,

(10) 0.092+0.45+8×0.016 =0.67<2
(1−0.092)⁢(1−0.45) =0.4994>0.016×8=0.128

It follows that conditions ( 8 ) are verified. From Theorem 2 and ( 10 ) it follows that the following iterative process

x1(i) =0.02⁢x1(i−1)+0.045⁢x2(i−1)+8⁢x3(i−1)+0,4
x2(i) =0.05⁢x1(i−1)+0.042⁢x2(i−1)+3⁢x3(i−1)−0,6
x3(i) =0.003⁢x1(i)+0.013⁢x2(i)+0,45⁢x3(i−1)−0.8,i=1,2,…

x10,x20,x30arbitrary, converges to the solution of the system ( 5 ).

By performing the calculations we verify all previous theoretical conclusions and after about 40 iterations we obtain the following approximate solution

x1 ≈−13.6542065,
x2 ≈−6.6168795,
x3 ≈−1.6854203.

Bibliography


Received on 12.VII.1969.

[1] I. Pavaloiu, Observatii asupra rezolvarii sistemelor de ecuatii cu ajutorul procedeelor iterative, Studii si Cercetari Matematice, 19 (1967) no. 9, 1289–1298 (in Romanian) [English translation of the title: Remarks on solving the systems of equations by iterative methods].

1969

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