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Error Inequalities for a Generalized Quadrature Rule

Nenad Ujevi´ c

Dedicated to Professor Dumitru Acu on his 60th anniversary

Abstract

Error inequalities for a generalized quadrature rule are derived.

A summation formula for the special function Si(x) is given.

2000 Mathematics Subject Classification: 26D15, 65D30.

Keywords: quadrature rule, generalization, numerical integration, error bounds.

1 Introduction

In recent years a number of authors have considered generalizations of some known and some new quadrature rules. For example, generalizations of the trapezoid, mid-point and Simpson’s quadrature rules are considered in [1],

51

(2)

[2], [3], [5] and [9]. As an illustration we give a generalization of the mid- point quadrature rule (see [3]),

Z b

a

f(t)dt = Xn−1

k=0

1 + (−1)k (b−a)k+1

2k+1(k+ 1)!f(k)(a+b

2 )+(−1)n Z b

a

Kn(t)f(n)(t)dt, where

Kn(t) =



(t−a)n

n! , t a,a+b2

(t−b)n

n! , t∈ a+b2 , b . Forn = 1 we get the mid-point rule

Z b

a

f(t)dt= (b−a)f(a+b 2 )

Z b

a

K1(t)f0(t)dt.

In this paper we consider a generalization of a simple quadrature rule of open type which has the form

(1)

Zb

a

f(t)dt= b−a 2

f(3a+b

4 ) +f(a+ 3b 4 )

+R(f).

In [14] it is shown that the above 2-point quadrature rule of open type is optimal with respect to a given way of estimation of the remainder term (error)R(f). We have (see [14])

(2) |R(f)| ≤ Γ−γ

16 (b−a)2, whereγ ≤f0(t)Γ, t∈[a, b].

On the other hand, the well-known 2-point Gauss quadrature rule (3)

Zb

a

f(t)dt = b−a 2

"

f(a+b

2

3

6 (b−a)) +f(a+b

2 +

3

6 (b−a))

#

+R1(f)

(3)

has the estimation of the error (see [10])

(4) |R1(f)| ≤ Γ−γ

24 (52

3)(b−a)2. Since 161 = 0.062 5 < 241 (52

3) = 0.063 99 we conclude that (2) is better than (4).

In [14] we can also find various error inequalities for this rule. Here we also give various error bounds for the generalization of this rule. These error bounds are generalizations of the error bounds obtained in [14] and they are similar to error bounds obtained in [15].

Finally, we give a numerical example. In fact, we derive a summation formula for the special function Si(x) =Rx

0 sint t dt.

2 Main results

Lemma 1. Let f : [a, b] R be a function such that f(n−1) is absolutely continuous. Then

(5)

Z b

a

f(x)dx= b−a 2

f(3a+b

4 ) +f(a+ 3b 4 )

−2 Xm

i=1

(b−a)2i+1 42i+1(2i+ 1)!

f(2i)(3a+b

4 ) +f(2i)(a+ 3b 4 )

+R(f), where m =n−1

2

, the integer part of (n1)/2,

(6) R(f) = (−1)n

Z b

a

Sn(t)f(n)(t)dt and

(7) Sn(t) =









1

n!(t−a)n, t∈

a,3a+b4

1

n! t− a+b2 n

, t∈ 3a+b4 ,a+3b4

1

n!(t−b)n, t∈a+3b

4 , b .

(4)

Proof. We prove (5) by induction. First we note that

S1(t) =









t−a, t∈

a,3a+b4 t− a+b2 , t∈ 3a+b4 ,a+3b4 t−b, t∈a+3b

4 , b

is a Peano kernel for the quadrature rule of open type, that is, we have

Z b

a

S1(t)f0(t)dt=−f(3a+b4 ) +f(a+3b4 )

2 (b−a) +

Z b

a

f(t)dt.

We easily show that (5) holds for n= 2. Now suppose that (5) holds for an arbitrary n. We have to prove that (5) holds for n n+ 1. To simplify the proof we introduce the notations

(8) Pn(t) = (t−a)n

n! ,

(9) Qn(t) = 1

n!

t−a+b 2

n ,

(10) Rn(t) = (t−b)n

n! .

We see thatPn, Qn and Rn form Appell sequences of polynomials, that is Pn0(t) = Pn−1(t), Q0n(t) = Qn−1(t), R0n(t) = Rn−1(t),

P0(t) = Q0(t) = R0(t) = 1.

We have

(−1)n+1 Z b

a

Sn+1(t)f(n+1)(t)dt

(5)

= (−1)n+1 Z 3a+b

4

a

Pn+1(t)f(n+1)(t)dt+ (−1)n+1 Z a+3b

4

3a+b 4

Qn+1(t)f(n+1)(t)dt (−1)n+1

Z b

a+3b 4

Rn+1(t)f(n+1)(t)dt

= (−1)n+1

Pn+1(3a+b

4 )f(n)(3a+b

4 )−Pn+1(a)f(n)(a)

+(−1)n+1

Qn+1(a+ 3b

4 )f(n)(a+ 3b

4 )−Qn+1(3a+b

4 )f(n)(3a+b 4 )

+(−1)n+1

Rn+1(b)f(n)(b)−Rn+1(a+ 3b

4 )f(n)(a+ 3b 4 )

+(−1)n Z 3a+b

4

a

Pn(t)f(n)(t)dt+ (−1)n Z a+3b

4

3a+b 4

Qn(t)f(n)(t)dt +(−1)n

Z b

a+3b 4

Rn(t)f(n)(t)dt

= (−1)n Z b

a

Sn(t)f(n)(t)dt +(−1)n+1

Pn+1(3a+b

4 )−Qn+1(3a+b 4 )

f(n)(3a+b 4 ) +(−1)n+1

Qn+1(a+ 3b

4 )−Rn+1(a+ 3b 4 )

f(n)(a+ 3b 4 )

= −f(3a+b4 ) +f(a+3b4 )

2 (b−a) +

Z b

a

f(t)dt

+ Xm

i=1

2(b−a)2i+1 42i+1(2i+ 1)!

f(2i)(3a+b

4 ) +f(2i)(a+ 3b 4 )

+(−1)n+1

Pn+1(3a+b

4 )−Qn+1(3a+b 4 )

f(n)(3a+b 4 )

(6)

+(−1)n+1

Qn+1(a+ 3b

4 )−Rn+1(a+ 3b 4 )

f(n)(a+ 3b 4 )

= −f(3a+b4 ) +f(a+3b4 )

2 (b−a) +

Z b

a

f(t)dt +

m1

X

i=1

2(b−a)2i+1 42i+1(2i+ 1)!

f(2i)(3a+b

4 ) +f(2i)(a+ 3b 4 )

wherem1 =n

2

, since

+(−1)n+1

Pn+1(3a+b

4 )−Qn+1(3a+b 4 )

f(n)(3a+b 4 ) +(−1)n+1

Qn+1(a+ 3b

4 )−Rn+1(a+ 3b 4 )

f(n)(a+ 3b 4 )

= (b−a)n+1 4n+1(n+ 1)!

1(−1)n+1

f(n)(3a+b

4 ) +f(n)(a+ 3b 4 )

.

This completes the proof.

Lemma 2. The Peano kernels Sn(t), n >1, satisfy:

(11)

Z b

a

Sn(t)dt= 0, if n is odd,

(12)

Z b

a

|Sn(t)|dt = (b−a)n+1 4n(n+ 1)!,

(13) max

t∈[a,b]|Sn(t)|= (b−a)n 4nn! . Proof. A simple calculation gives

Z b

a

Sn(t)dt = 2(b−a)n+1 4n+1(n+ 1)!

1(−1)n+1 .

(7)

From the above relation we see that (11) holds, since 1(−1)n+1 = 0 if n is odd.

We now consider some properties of the Appell sequences of polynomials Pn(t), Qn(t) and Rn(t), given by (8), (9) and (10), respectively. We have that (t−a)n 0, for eachn, such thatPn(t)0,∀nandt

a,3a+b2

. Since Pn0(t) =Pn−1(t) we conclude thatPn(t) are increasing functions. Ifnis even then t− a+b2 n

0. If n is odd then t−a+b2 n

0, for t∈a+b

2 a+3b 4

and t− a+b2 n

0, for t∈3a+b

4 ,a+b2 .

Since Q0n(t) = Qn−1(t) we conclude that Qn(t) is increasing function if n is even andQn(t) is decreasing function fort∈3a+b

4 ,a+b2

, whileQn(t) is increasing function for t∈a+b

2 a+3b

4

, if n is odd.

We have that (t−b)n 0 if n 1, n is odd and (t−b)n 0 if n 0, n is even. Thus, we have that Rn(t) 0 if n is odd and Rn(t) 0 if n is even. As we knowRn0(t) = Rn−1(t) such thatRn(t) are decreasing functions if n is even and Rn(t) are increasing functions if n is odd. We use these properties to prove (12) and (13).

We have

Z b

a

|Sn(t)|dt =

Z 3a+b

4

a

|Pn(t)|dt+ Z a+3b

4

3a+b 4

|Qn(t)|dt+ Z b

a+3b 4

|Rn(t)|dt

= (b−a)n+1 4n(n+ 1)!.

(8)

Finally, we have

t∈[a,b]max|Sn(t)| = max (

max

t∈[a,3a+b4 ]|Pn(t)|, max

t∈[3a+b4 ,a+3b4 ]|Qn(t)|, max

t∈[a+3b4 ,b]|Rn(t)|

)

= max

Pn(3a+b 4 )

,

Qn(3a+b 4 )

,

Qn(a+ 3b 4 )

,

Rn(a+ 3b 4 )

= (b−a)n 4nn! . We introduce the notations

I = Z b

a

f(t)dt,

F = −f(3a+b4 ) +f(a+3b4 )

2 (b−a)

+ Xm

i=1

2(b−a)2i+1 42i+1(2i+ 1)!

f(2i)(3a+b

4 ) +f(2i)(a+ 3b 4 )

.

Theorem 3. Let f : [a, b] R be a function such that f(n−1), n > 1, is absolutely continuous and there exist real numbers γn,Γn such that γn f(n)(t)Γn, t∈[a, b]. Then

(14) |I−F| ≤ 1 2

Γn−γn (n+ 1)!

1

4n(b−a)n+1 if n is odd and

(15) |I−F| ≤ (b−a)n+1n 4n(n+ 1)!

f(n)

if n is even.

Proof. Letn be odd. From (6) and (11) we get R(f) = (−1)n

Z b

a

Sn(t)f(n)(t)dt= (−1)n Z b

a

Sn(t)

f(n)(t) γn+ Γn 2

dt

(9)

such that we have

(16) |R(f)|=|I−F| ≤ max

t∈[a,b]

f(n)(t) γn+ Γn 2

Z b

a

|Sn(t)|dt.

We also have

(17) max

t∈[a,b]

f(n)(t) γn+ Γn 2

Γn−γn

2 .

From (16), (17) and (12) we get

|I−F| ≤ 1 2

Γn−γn (n+ 1)!

1

4n(b−a)n+1. Letn be even. Then we have

|R(f)|=|I−F| ≤ Z b

a

|Sn(t)|dt f(n)

= (b−a)n+1n 4n(n+ 1)!

f(n) .

Theorem 4. Let f : [a, b] R be a function such that f(n−1), n > 1, is absolutely continuous and letn be odd. If there exists a real number γn such that γn≤f(n)(t), t∈[a, b] then

(18) |I −F| ≤(Tn−γn)(b−a)n+1 4nn! , where

Tn= f(n−1)(b)−f(n−1)(a)

b−a .

If there exists a real number Γn such that f(n)(t)Γn, t∈[a, b] then (19) |I −F| ≤n−Tn)(b−a)n+1

4nn! . Proof. We have

|R(f)|=|I−F|=

Z b

a

(f(n)(t)−γn)Sn(t)dt ,

(10)

since (11) holds. Then we have

Z b

a

(f(n)(t)−γn)Sn(t)dt

max

t∈[a,b]|Sn(t)|

Z b

a

(f(n)(t)−γn)dt

= (b−a)n 4nn!

f(n−1)(b)−f(n−1)(a)−γn(b−a)

= (b−a)n+1

4nn! (Tn−γn). In a similar way we can prove that (19) holds.

Remark 5. Note that we can apply the estimations (14) and (15) only if f(n) is bounded. On the other hand, we can apply the estimation (18) if f(n) is unbounded above and we can apply the estimation (19) if f(n) is unbounded below.

3 A numerical example

Here we consider the integral (special function) Si(x) =Rx

0 sint

t dt and apply the summation formula (5) to this integral. We get the summation formula Si(x) = F(x) +R(x), where

(20) F(x) = 2 sinx 4 + 2

3sin3x 4 +

Xm

i=1

2x2i+1 42i+1(2i+ 1)!

f(2i)(x

4) +f(2i)(3x 4 )

and f(t) = (sint)/t. We calculate the derivatives f(j)(t) as follows. We have

(g(t)h(t))(j) = Xj

k=0 j k

g(k)(t)h(j−k)(t).

(11)

If we choose g(t) = sint and h(t) = 1/t then we get f(j)(x

4) = [Xj−12 ]

i=0 j 2i+1

(−1)j−i+1(j2i1)!4j−2i xj−2i cosx

4 +

[2j] X

i=0 j 2i

(−1)j−i(j 2i)!4j−2i+1 xj−2i+1 sinx

4,

f(j)(3x 4 ) =

[Xj−12 ]

i=0 j 2i+1

(−1)j−i+1(j2i1)!4j−2i

3j−2ixj−2i cos3x 4 +

[2j] X

i=0 j 2i

(−1)j−i(j2i)!4j−2i+1

3j−2i+1xj−2i+1 sin3x 4 .

We now compare the summation formula (20) with the known compound formula (for the given quadrature rule of open type),

(21)

Z x

0

f(t)dt = h 2

Xn−1

i=0

f(3xi+xi+1

4 ) +f(xi+ 3xi+1

4 )

+R(x), where xi =ih, h=x/n, f(t) = (sint)/t.

Let us choose x = 1. The ”exact” value is Si(1) = 0.946083070367. If we use (20) withm = 5 then we get Si(1)≈0.946083070363. If we use (21) with n = 40000 then we get Si(1) ≈ 0.946083070369. All calculations are done in double precision arithmetic. The first approximate result is obtained much faster than the second approximate result. The same is valid if we use some quadrature rule of higher order, for example Simpson’s rule. This is a consequence of the fact that we have to calculate the function sint many times when we apply the compound formula and we have only to calculate sin(x/4),cos(x/4), sin(3x/4) and cos(3x/4) when we apply the summation formula.

(12)

Similar summation formulas can be obtained for the integrals (special functions): Rx

0 [(et1)/t]dt, Rx

0 [(cost−1)/t]dt, Rx

0 exp(−t2)dt, etc.

References

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[3] P. Cerone and S. S. Dragomir, Trapezoidal-type Rules from an Inequal- ities Point of View, Handbook of Analytic-Computational Methods in Applied Mathematics, Editor: G. Anastassiou, CRC Press, New York, (2000), 65–134.

[4] D. Cruz-Uribe and C. J. Neugebauer,Sharp error bounds for the trape- zoidal rule and Simpson’s rule, J. Inequal. Pure Appl. Math., 3(4), Article 49, (2002), 1–22.

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Math. Comput., 123 (2001), 37–62.

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are bounded and applications in numerical integration and for special means, Appl. Math. Lett., 13 (2000), 19–25.

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[8] D. S. Mitrinovi´c, J. Peˇcari´c and A. M. Fink, Classical and new in- equalities in analysis, Kluwer Acad. Publ., Dordrecht/Boston/London, 1993.

[9] C. E. M. Pearce, J. Peˇcari´c, N. Ujevi´c and S. Varoˇsanec, General- izations of some inequalities of Ostrowski-Gr¨uss type, Math. Inequal.

Appl., 3(1), (2000), 25–34.

[10] N. Ujevi´c,Inequalities of Ostrowski-Gr¨uss type and applications, Appl.

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[11] N. Ujevi´c, A generalization of Ostrowski’s inequality and applications in numerical integration, Appl. Math. Lett., 17(2), (2004), 133-137.

[12] N. Ujevi´c, New bounds for the first inequality of Ostrowski-Gruss type and applications, Comput. Math. Appl., 46, (2003), 421-427.

[13] N. Ujevi´c and A. J. Roberts, A corrected quadrature formula and ap- plications, ANZIAM J., 45(E), (2004), E41–E56.

[14] N. Ujevi´c,Error inequalities for an optimal 2-point quadrature formula of open type, (to appear in ”Inequality Theory and Applications”, Nova Science Publishers, Inc., New York).

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[15] N. Ujevi´c, Error inequalities for a generalized trapezoid rule, Appl.

Math. Lett, (in press).

Department of Mathematics University of Split

Teslina 12/III, 21000 Split CROATIA

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