Atakut and Ibrahim Büyükyaz?c?
Ankara University,Faculty of Science,Department of Mathematics,06100 Tandogan,Ankara,Turkey
Abstract.In the present paper,we deal with Chlodowsky type generalization of the Baskakov operators,special case of these operators includes Chlodowsky type Meyer–K?nig and Zeller operators(see[21]). With the help of Bohman-Korovkin theorem,we obtain some approximation properties for these operators.We give a modification of the operators in the space of differentiable functions and we also present examples of graphs for approximation.Finally,we apply these operators to the solution of the differential equation.
Key Words:Approximation properties,Rate of convergence,Chlodowsky type MKZ operators,Baskakov operators,Differential equation.
Let{?n}(n=1,2,···),be a sequence of functions,having the following properties:
i)?nis analytic on a domain D containing the diskfor each positive integer n,
ii)?n(0)=1 for n∈N,
iii)?n(x)>0 andfor every positive integer n,x ∈[0,∞)and and for every nonnegative integer k.
In[5],V.A.Baskakov introduced following the sequence of linear operators{Ln},
Furthermore,if we take ?n(x)=(1+x)nand replace x by anx in the operator(1.1),we have
This operator is known as Bernstein type rational function which was studied in[4,16].
where for 0
Motivated by this work,we give Chlodowsky type generalization of Ln(f;x)operators given by(1.2)as follows:
and γ be real number in the intervalAssume that the sequence of functions{?n}satisfies the conditions(i)-(iv).For a function f defined on[0,∞)and bounded on every finite interval[0,γ],we define the following sequence of linear positive operators:
Recently,linear positive operators and their Chlodowsky type generalizations have been widely studied by several authors[1,3–22],because this generalization allows us to investigate approximation properties of functions defined on the infinite interval[0,∞)by using the similar techniques and methods on the classical operators.
The aim of this paper is to study some convergence properties of the operators Ln(f;βn,x)defined by(1.4)and modify the operators for differentiable functions,in order to improve the rate of convergence on the interval[0,βn]extending infinity as n→∞.Also we give an application to functional differential equation by using these operators.
In this section we study conditions of Korovkin theorem[2]and the rate of convergence,an asymptotic formula for the operators(1.4)for f ∈C[0,γ].
Now we use the test functions ei(t)=ti,i=0,1,2.Then,we obtain the following result.
Theorem 2.1.Let{βn}be a positive increasing sequence satisfying(1.3)and the operators Ln(f;βn,x)be defined by(1.4)with the conditions(i)-(iv).For every finite intervaland for eachwe have
Proof.Firstly,from condition(i),we have
so we get
By the definition of the operators(1.4)and using e1(t)=t
by(iv),we have
or
On the other hand,observe that
combining(2.2)with(2.3),we have
and hence,
uniformly in[0,γ].
Finally,for e2(t)=t2,we obtain
by(iv),we get
using this equalities,we obtain
which implies that
on the other hand,it is clear that Ln(e2(t);βn,x)?e2(x)≥0.Using(2.4),we get
Hence we have
uniformly in[0,γ].Thus,the proof of the theorem is completed.
Remark 2.1.LetSimple calculations,one can easily obtain ψn=1,αn,k=0.Then Ln(f;βn,x)has the following form:
Chlodowsky type MKZ operators(see[21]).
Example 2.1.For n=10,50 andthe convergence of Ln(f;βn,x)to f(x)will be illustrated in Fig.1 and Fig.2.
Example 2.2.Let n=10.For βn=n4/5and βn=n2/3,the convergence of Ln(f;βn,x)to f(x)will be illustrated in Fig.3.
Figure 1:The convergence of Chlodowsky type MKZ operators to f(x)=x1/3.
Figure 2:The convergence of Chlodowsky type MKZ operators to
Figure 3:The convergence of Chlodowsky type MKZ operators to
Now we give the approximation order of operators(1.4)with help of asymptotic inequality.
Let I=[0,γ]and C(I)be the space of all continuous functions f.For a fixed r∈N we denote by
Theorem 2.2.If the operators Lnare defined by(1.4),then for sufficiently large n and for every f ∈C2(I)
Proof.By the Taylor formula,we write
where λ(t)→0 as t→x.If we Apply the operators(1.4)to(2.5),we get
From(2.1),(2.2)and(2.4),we have
using(2.7a)-(2.7c)in(2.6),one obtains
and hence
which implies
Thus the desired result is obtained.
In recent years several authors[7,8,17,21,22]investigated approximation properties of certain linear operators for differentiable functions.In this section we will modify the operator(1.4)for differentiable functions,in order to improve the rate of convergence of the sequence{Lnf}to f(see Example 3.1)
Theorem 3.1.Ifthen
where B(α,r)is a beta function and Lnis defined by(1.4).
Proof.From(2.1),we can write
Consider the term in parentheses.Using modified Taylor’s formula we have
since f(r)∈LipMα,we obtain
On the other hand,we have
where B(α,r)is a beta function.Therefore we write
from(3.1)and(3.2),we have
Thus the proof of theorem is completed.
Remark 3.1.If we choosewe obtain Chlodowsky type generalized MKZ operators defined by
(see[21]).
Example 3.1.For n=10,βn=n2/3and r=2,the convergence comparison ofand Ln(f;βn,x)to f(x)will be illustrated in Fig.4 and Fig.5.
Example 3.2.Let n=10.For βn=n4/5and βn=n2/3,the convergence ofto f(x)=x6will be illustrated in Fig.6
Many authors obtained some differential equations by using the linear positive operators which are solution of these equations,we refer the readers to[1,3,8,9,19].In this section,using the same idea and method,as an application to the differential equation,we obtain a functional differential equation so that the linear positive operator Ln(f;βn,x)is a particular solution of it.
Figure 4:Comparison Chlodowsky type MKZ operators and Chlodowsky type MKZ-Taylor operators for f(x)=
Figure 5:Comparison Chlodowsky type MKZ operators and Chlodowsky type MKZ-Taylor operators for f(x)=
Figure 6:The convergence of Chlodowsky type MKZ–Taylor operators to f(x)=x6.
Theorem 4.1.LetFor each x ∈[0,γ]and f ∈C[0,γ],the operators Ln(f;βn,x)defined by(1.4)satisfy the following differential equation:
where
Proof.By the Theorem 2.1,if f ∈C(I),then Ln(f;βn,x)converges uniformly to f(x)on[0,γ].So we can differentiate both sides of(1.4)term by term to obtain
Thus we can see that:
and
hence we get
This gives the desired result.
Corollary 4.1.The operators Ln(f;βn,x)given by(1.4)are a particular solution of the following differential equation:
where βnis given by(4.2).
Proof.Selecting f(t)=βn?t in(4.1),we get
from(2.1),we have
which gives the proof.
Analysis in Theory and Applications2018年4期