Abstract
We consider optimality problems regarding the order of convergence of the iterative methods which are obtained by inverse interpolation of Lagrange-Hermite type. A similar problem for a class of Steffensen-type methods is solved.
Authors
Ion Păvăloiu
(Tiberiu Popoviciu Institute of Numerical Analysis)
Title
Optimal problems concerning interpolation methods of solution of equations
Keywords
nonlinear equations in R; order of convergence; iterative methods; inverse interpolation; Lagrange-Hermite; Steffensen-type methods.
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I. Păvăloiu, Optimal problems concerning interpolation methods of solution of equations, Publications de L’Institut Mathématique (Nouvelle série) Beograd, 52(66) (1992), pp. 113-126
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References
[1] C. Iancu, I. Pavaloiu, La resolution des equations par interpolation inverse de type Hermite, Mathematica 26(49) (1984) no. 2, 115–123.
[2] C. Iancu, I. Pavaloiu, I. Serb. Methodes iteratives optimales de type Steffensen obtenues par interpolation inverse, Research Seminar on Functional analysis and Numerical Methods, Preprint 1 (1983), 81–88.
[3] M. A. Ostrowski, Solution of Equations and Systems of Equations, Academic Press, New York and London, 1980.
[4] I. Pavaloiu, Solving the Equations by Interpolation, Dacia, Cluj-Napoca, 1981, (in Romanian).
[5] J.F. Steffensen, Interpolation, Chelsea Publ., New York, 1950.
[6] J.F. Traub, Iterative Methods for the Solution of Equation, Prentice-Hall, Englewood Cliffs, N.J., 1964.
[7] B.A. Turowicz, Sur les deriv´ees d’ordre superiour d’une fonction inverse, Ann. Polon. Math. 8 (1960), 265–269.
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PUBLICATIONS DE L’INSTITUT MATHÉMATIQUE
Nouvelle série tome 52(66), 1992, 113–126
Optimal Problems Concerning Interpolation Methods of Solution of Equations
Abstract.
We consider optimality problems regarding the order of convergence of the iterative methods which are obtained by inverse interpolation of Lagrange-Hermite type. A similar problem for a class of Steffensen-type methods is solved.
Introduction
The inverse interpolation problem, connected with equation solution was essentially approached in [5], [6], [7], [4]. In [4] it was shown that the most known iteration methods, are: Newton’s method, Chebyshev’s method, chord method, as well as various generalizations of them, which are all obtained by means of Lagrange-Hermite-type inverse interpolations. A classification of these methods according to their order of convergence is not beyond interest. In this paper we propose to solve two extremum problems concerning the order of convergence of the iteration methods obtained by the Lagrange-Hermite-type inverse interpolation and that of the Steffensen-type method which follows from the preceding ones.
The Lagrange-Hermite-type inverse interpolation polynomial with nodes each node having a given multiplication order, leads to a class of iteration methods. Out of this class of methods, we propose to determine the method having the highest order of convergence. In the last part of the paper we solve the same problem for a class of Steffensen-type iteration methods.
1. The inverse interpolation problems and the determination of optimal iteration method
Let be a function, where is an interval of the real axis. Denote by a set of distinct points from the interval , namely where for .
Consider the natural numbers and suppose that they satisfy
(1.1) |
It is a well-known fact that the numbers being given, there exists a unique polynomial , of degree at most , which satisfies the relations
(1.2) |
The polynomial satisfying the conditions (1.2) has the form:
(1.3) |
where:
(1.4) |
If we suppose that the function admits derivatives up to the order on the interval , and if we put in (1.3), then is the Hermite interpolating polynomial on the nodes , associated with the function , and the following equality holds:
(1.5) |
with .
We shall suppose, in what follows, that for every and denote . It follows that is bijective, hence there exists and the function admits derivatives up to the order, for every .The order derivative, where can be determined by means of the following formula [7]:
(1.6) |
where the above sum is extended over all integral and nonnegative solutions of the system
(1.7) | ||||
If we suppose that the equation:
(1.8) |
admits a root , then the hypothesis for every leads to the conclusion that this root is unique.
From it follows that and the problem of the approximate solution of the equation (1.8) reduces to the determination of an approximation for . Let be a function which approximates the function , at least in a neighbourhood of the point ; thus an approximation formula of the form:
(1.9) |
holds on the set .
Neglecting the function and putting into (1.9), we obtain the following approximation for :
(1.10) |
with an approximation error given by the inequality
(1.11) |
There are two natural conditions to be imposed on the function :
-
a)
to approximate the function as well as possible, i.e. the number must be as small as possible;
-
b)
to have some simplicity properties for the computation of its values.
The functions which agree with the second condition are (or rather seem so) polynomials, since the computation of their values reduces to elementary arithmetic operations.
Obviously, if we succeed in constructing the best approximating polynomial for on the set , then the first condition will be satisfied too.
In what follows we shall not approach the problem from this point of view; therefore the function will be replaced by the Hermite interpolating polynomial associated to the function , on the set , called Hermite inverse interpolating polynomial. For this purpose, in the interpolating polynomial (1.3) we consider, as interpolating nodes, the values , while for , we consider respectively . In this way the polynomial (1.3) acquires the form:
(1.12) |
where:
(1.13) |
From (1.5) it follows that
(1.14) |
Taking into account the fact that from (1.14) one obtains:
(1.15) |
where is a point lying in the shortest interval which contains Denoting this interval by and putting:
(1.15′) |
it results, from (1.15),
(1.16) |
and since ,
(1.17) |
From (1.17) it follows that if are chosen sufficiently close to , then the values are real numbers close to zero; so much more the product will be close to zero. This remark allows us to consider the value as an approximation for the root of the equation (1.8).
If is not a good enough approximation for , then we can construct, by iterations, a sequence of approximations , which, under certain conditions, will be convergent, and .
More precisely, let be approximations of the root of the given equation (1.8). We denote and replace one of the nodes , then continue the iteration process by the above described procedure.
The problem which arises is to determine the interpolating node which should be replaced at each iteration step in order to obtain a sequence of approximations with a maximum order of convergence. To solve the problem, let us consider the following equations:
(1.18) | ||||
(1.19) | ||||
(1.20) |
where a are real numbers satisfying the conditions:
(1.21) | ||||
(1.22) |
while is an arbitrary permutation of the numbers .
The following lemma holds:
Lemma 1.
If satisfy the condition (1.21), then any of the equations (1.20) has a single positive and supraunitary root. If, it addition, the condition (1.22) is also satisfied and we denote by respectively, the positive roots of the equations (1.18)–(1.20), then
(1.23) |
i.e. the equation (1.18) admits the greatest root.
Proof.
Consider one of the equations of the form (1.20) and denote by the greatest natural number for which . We have and consider the function . We have , and . Accordingly, the equation has at least one supraunitary root and therefore has at least one supraunitary root.
The uniqueness of this root follows easily if we consider the function which satisfies the condition for .
In order to prove the inequalities (1.23) it is sufficient to show that and . Indeed, we have:
since and .
The inequality can be proved analogously. ∎
Consider now the permutation of the numbers for which the natural numbers satisfying the equality (1.1), can be increasingly ordered, namely:
(1.24) |
We renumber, accordingly, the elements of the set i.e. we consider:
For the sake of clearness we shall set:
(1.25) |
and
(1.26) |
and denote by the Hermite interpolating polynomial, corresponding to the nodes having the multiplicities respectively.
Let be the initial approximations of the root of the equation (1.8). We construct the sequence by means of the following iterative procedure:
(1.28) |
Denoting and we obtain from (1.27) and (1.28):
(1.29) |
Denoting we obtain from (1.29):
(1.30) |
Suppose that there exists a , , such that:
where is the positive root of the equation (1.18). That number is called the convergence order of the method (1.28).
If we suppose that:
then, taking into account (1.30) and the fact that is a root of the equation (1.18), we derive the inequality:
(1.31) |
which is valid for every
Taking into account the expression for , we obtain the following inequality for the error evaluation:
(1.32) |
from which it follows that .
Observe that both the error evaluation and the convergence speed of the method (1.28) depend on the root of the equation (1.18). The greatest is, the better the upper limit obtained for the error is.
Consider all permutations of the set To each permutation it corresponds an iterative method of the form:
(1.33) |
All together we have iterative methods.
Taking into account Lemma 1 and the results proved so far, we can state the following theorem:
Theorem 1.
Out of the iterative methods of the form (1.33), with the greatest convergence order (namely these which provide the best upper limit for the absolute value of the error) is that determined by the permutation which orders increasingly the numbers namely .
2. Some particular cases
In what follows we shall discuss some particular cases.
Case From (1.12) one obtains the Taylor inverse interpolating polynomial:
(2.1) |
while, from (1.6), we obtain the following expressions for the successive derivatives
(2.2) |
(2.3) |
(2.4) |
(2.5) |
From (2.2) and (2.1) for we obtain:
which, for leads to the approximation of given by expression
(2.6) |
i.e. to the Newton’s method.
From the above methods one obtains by iterations the corresponding sequence of approximations, which has the order of convergence 2, 3 and 4 respectively.
As one may notice from (2.5) and (1.6), for the expressions for the derivatives have a more complex form. That is why the methods following from (2.1) in these cases are also complex.
Case In this case, from (1.12) it follows:
(2.9) |
where:
(2.10) |
From (2.9) one obtains two iterative methods; namely denoting as above by the Hermite inverse interpolating polynomial (2.9), we find:
(2.11) |
or
(2.12) |
The characteristic equations which provide the convergence orders for the two methods are
(2.13) |
for the method (2.11), and:
(2.14) |
for the method (2.12).If we denote by and , respectively, the positive roots of equations (2.13) and (2.14), then it is clear that implies so, the method with optimal convergence order is the method (2.11).
Now, we shall briefly discuss some particular cases.
From (2.9), for we obtain
(2.15) |
wherefrom, taking into account the fact that and , we find for
(2.16) |
where stands for the first order divided difference of the function on the nodes and , and
(2.17) |
which is the chord method. In this case, since the above method has the same convergence order as the other one, which follows from (2.12), i.e.:
(2.18) |
The order of convergence of the method (2.17) is
Now we shall discuss the case . In this particular case, we obtain from (2.9) the following iterative methods:
(2.19) | ||||
and
(2.20) | ||||
Solving the corresponding characteristic equations, we find the convergence orders for the method (2.19) and for the method (2.20).
As we showed above, the Hermite inverse interpolating polynomial leads to a large class of iterative methods. The convergence order of each method depends on the number of interpolating nodes, the order of multiplicity of these ones, and, essentially, on the interpolating node replaced at each iteration step by that calculated at the precedent one.
As Steffensen notices, in the case of the method (2.17), the convergence order of this method can be increased if at each iteration step the element depends in a certain manner on . More exactly, if we consider a function , having the property , where is the root of the equation (1.8), and if we put into (2.17), then we obtain the sequence generated by Steffensen’s method:
which has, as it is well known, the convergence order 2.
3. Steffensen-type optimal methods
Now let , be functions satisfying the following conditions:
-
a)
, where
-
b)
there exist real numbers and such that the functions and satisfy the relations:
(3.1)
Denote by an initial approximation of the root of the equation (1.8).
We construct interpolating nodes as follows:
(3.2) |
Denote , and consider the natural numbers satisfying:
(3.3) |
Using the interpolating nodes and the Hermite interpolating polynomial on these nodes, with the orders of multiplicity , respectively, we obtain, for the following approximations:
(3.4) |
with the error evaluation given by the inequality:
(3.5) |
where
(3.6) |
Now, using the property b) of the function , we derive
and generally,
(3.7) |
If we denote
(3.8) |
and
(3.9) |
having in view (3.6) and (3.7), we obtain:
(3.10) |
wherefrom, taking into account (3.5), we derive
(3.11) |
If we consider now some element that we have constructed by iterations, then the interpolating nodes corresponding to the next step are obtained, as in the case of the first step, by using the relations:
(3.12) |
Constructing the element , as for the first step, we obtain:
(3.13) |
where , which infers the following inequality
(3.14) |
Denoting the inequalities (3.14) take the form
wherefrom we derive
(3.15) |
where
If we assume that
(3.16) |
then, from (3.15), it follows
(3.17) |
Let and be two arbitrary permutations of numbers . Also denote
the Hermite inverse interpolating polynomial having the interpolating nodes with the orders of multiplicity .
With the above denotations, let us consider the following class of iterative methods
(3.18) |
where
and
(3.19) | ||||
being the given initial approximation.
To each couple of permutations and of the numbers there corresponds an iterative method of the form (3.18).
All together we have again iterative methods of this form.
We shall attempt to determine, out of the iterative methods, that one for which the number given by (3.8) is maximum.
With this goal in view, we shall first prove the following lemma:
Lemma 2.
Let with with , be real numbers satisfying
(3.20) |
Out of all numbers of the form
(3.21) |
where and arbitrary permutations of the set , the greatest one is the number
(3.22) |
Proof.
From the first set of inequalities (3.20) it follows that the inequality:
(3.23) | ||||
holds for any two permutations and of the numbers .
Let us denote
(3.24) |
and let us attempt to prove the inequality
(3.25) |
for every permutation . We shall do that by induction. For the inequality (3.25) is obvious, since and hence . Suppose now that the inequality is true for pairs of numbers namely
(3.26) |
where and . Using the inequalities and , as well as the induction hypothesis (3.26), and assuming that , we have
∎
The above lemma leads to the following theorem:
Theorem 2.
References
- [1] ††margin: clickable C. Iancu, I. Păvăloiu, La résolution des équations par interpolation inverse de type Hermite, Mathematica 26(49) (1984) no. 2, 115–123.
- [2] ††margin: clickable C. Iancu, I. Păvăloiu, I. Serb. Methodes itératives optimales de type Steffensen obtenues par interpolation inverse, Research Seminar on Functional analysis and Numerical Methods, Preprint 1 (1983), 81–88.
- [3] M. A. Ostrowski, Solution of Equations and Systems of Equations, Academic Press, New York and London, 1980.
- [4] I. Păvăloiu, ††margin: clickable Solving the Equations by Interpolation, Dacia, Cluj-Napoca, 1981, (in Romanian).
- [5] J.F. Steffensen, Interpolation, Chelsea Publ., New York, 1950.
- [6] J.F. Traub, Iterative Methods for the Solution of Equation, Prentice-Hall, Englewood Cliffs, N.J., 1964.
- [7] B.A. Turowicz, Sur les derivées d’ordre superiour d’une fonction inverse, Ann. Polon. Math. 8 (1960), 265–269.
Academia Română (Received 22 05 1991)
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