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Tiberiu Popoviciu
Institutul de Calcul
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T. Popoviciu, Application de la théorie des fonctions convexes d’ordre supérieur à l’étude de certains procédés d’intégration numérique des équations différentielles, Folia Fac. Sci. Natur. Univ. Purkyhnianae Brunensis, Ser. Monograph., Tomus 1, Purkyne Univ., Brno, 1973, pp. 241-245 (in French).
Proceedings of Equadiff III (Third Czechoslovak Conf. Differential Equations and their Appl., Brno, 1972), Miloš Ráb and Jaromír Vosmanský (eds.).
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APPLICATION OF THE THEORY OF HIGHER ORDER CONVEX FUNCTIONS TO THE STUDY OF CERTAIN PROCESSES OF NUMERICAL INTEGRATION OF DIFFERENTIAL EQUATIONS
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1.
Most of the linear approximation formulas involved in the numerical integration processes of differential equations can be put into the form
| (1) |
For specific formulas one can consult various books on numerical analysis and, in particular, the well-known book by L. Collatz [1].
Formula (1), also called a numerical derivation formula, allows us to approximately calculate the value of the derivative of a certain order (of order) of a function, on a given point (the point), by a given linear combination of the values, in finite number, of the function and of some of its successive derivatives, on given points. Theare given constants, the distinct pointsof the real axis belong to the bounded and closed intervalon which the functionis defined. Finally theare natural numbers andnon-negative integers also given.
The difference, between the first and second members of formula (1), is the remainder of this numerical derivation formula. In a previous work [3] we made a fairly detailed discussion of this remainder and later we completed these results [6].
2. Note that the remainderis a linear functional defined on a certain setof functionsdefined on the interval. The study of the rest, which obviously depends on the function, therefore of the structure of the whole, leads to various delimitations of the error committed by the approximation (1) of.
Let us assume that, in general,be a linear functional defined on a linear setof real and continuous functions, defined on an intervalof the real axis. The theory of higher-order convex functions or the theory of various generalizations of these functions can be used to specify the structure of the functionalwhen it has a degree of accuracy or something analogous.
Suppose, in particular, thatcontains all polynomials. Then the degree of exactness, if it exists, is an integerwell determined by the property that
is zero on any polynomial of degreeand is different from zero on at least one polynomial of degree). We then have the following theorem:
Whenis nonzero on any function, convex of order, We have
| (2) |
Oris independent of the functionand the knotsgenerally depend on the function, are distinct and even within the intervalif.
In this case we say that the linear functionalis of the simple form. Moreover, for simplicity, in a certain sense, the condition thatbe different from zero forconvex of a certain order, is at the same time necessary and sufficient. Various criteria allow us to decide whether a linear functionalis of the simple form or not. Of the simple form are the remainders in many linear approximation formulas of analysis. For example, in the Taylor formula, in the more general Lagrange-Hermite interpolation formula, in many classical mechanical quadrature formulas and in most linear formulas used in the numerical integration of differential equations. As for the factor, it is equal to.
I introduced (first under another name) the notion of linear functional of the simple form in another work [2].
The functionis said to be convex of orderonif all its differences divided, of orderon knotsdistinct, are positive.
For the definitions and properties of divided differences on distinct or non-distinct nodes, of higher-order convex functions, for the notion of simplicity of a linear functional and for various other properties used in this work, one can consult my previous works. For example, my dissertation of "Mathematica" [4].
Finally, let us note that, in the case of the simplicity of, formula (2) must be considered in close connection with various theorems and formulas of the mean of divided differences. The right-hand side of formula (2) can also be represented in various forms. For example, ifand if the functionhas a derivativeth on the inside of, We have
| (3) |
being a point of the interior of.
3. The linear functionalmay not be of the simple form, but if it
has a determined degree of accuracy,, under fairly general assumptions (see [4]), we have a formula of the form
| (4) |
Orare independent of the functionAnd,are two groups ofdistinct points of, generally depending on the function. We haveand the simplicity comes down to the fact that we can choose one of the coefficientsequal to zero. If the functionhas a derivativeth on the inside of, from (4) we deduce the formula
| (5) |
being two points of the interior of.
Note that this time instead of a single group of pointsrespectively of a single pointwe encounter two groups of points, respectively two points,, generally without connection between them, of the intervalof function definition.
The preceding considerations apply to a linear functional of the form
| (6) |
where the nodesare distinct and the coefficientsare independent of the function. Whenis not zero identically, so if theare not all zero, the linear functional has a degree of accuracywell determined.
In particular, the remainder of the approximation formula (1) is of the form (6).
Note also that by passing to a primitive of the function, the study of the remainder of a quadrature formula allowing the approximate calculation of an integral of the form, returns to the study of a functional of the form (6) (see [4]).
4. We have sought to remedy the defect highlighted by the italicized lines of the previous no.
Whenis not of the simple form we can seek to reestablish simplicity by defining a degree of simplicity not in relation to the successive powers of, but with respect to a suitably defined Tschebycheff system on. We have applied such a method in a previous work [5]. Assuming thathas a sufficient number of derivatives, we can then, in certain cases, obtainas a linear combination of the values ​​of some of the derivatives ofon a single point(generally depending on the function). This linear combination can have coefficients also depending on, as shown by the example of our cited work [5].
5. In the particular case of the linear functional (6) we can obtain such a formula also in the following way. We can find a function, defined on, depending only on the coefficientsand knots(hands not of the functionand functional), so that we have
| (7) |
The total number of nodes of the divided difference of the second member is. We can always find fora polynomial, even of degree. It is determined as a Lagrange-Hermite interpolation polynomial on thenodes considered.
So if we assume thatand thateither-times derivable (as well as) on the inside of, we get
| (8) |
being an interior point ofdepending, in general, on the functionThis result is obtained by taking into account the classical Cauchy formula
being inside the smallest interval containing the nodes.
6. The functionnot being determined in a unique way, there may be several representations of the previous form.
Example. Consider the linear functional
OrAndis continuous onand derivable on the open interval.
This linear functional is of the form
by choosing, or, or else.
Formula (8) gives us
We therefore obtain, either
either
In both formulas the numberis obviously not the same. To justify this statement it is enough to take.
BIBLIOGRAPHY
[1] Collatz, L.: Numerische Behandlung von Differentialgleichungen, 1955.
[2] Popoviciu, T.: Asupra former restului in unele formulae de aproximare ale analizei, Lucrările Ses. Gen. stiințifice ale Acad. RPR din 2-12 iu nie 1950, 183-186 (1950)
[3] Popoviciu T.: Asupra restului în unele formula de derivare numerică (On the remainder in some formulas of numerical derivation). Studii si Cercetări Matematice, T. III, 53-122 (1952)
[4] Popoviciu, T.: On the remainder in certain linear formulas of approximation of the analysis, Mathematica, 1 (24), 95-142 (1959)
[5] Popoviciu T.: On the remainder of certain quadrature formulas, Aequationes math., 2, 265-268 (1969)
[6] Popoviciu T.: Das Restglied in einigen Formeln der numerischen Integration von Differentialgleichungen, Methoden und Verfahren der Mathematischen Physik, B. 5, 117-129 (1971)
The author's address:
Tiberiu Popoviciu
Institutul de Calcul
37 Str. Republicii, Cluj
Romania
