Wave Scattering by Small Bodies of Arbitrary Shapes

A.5: Optimal Methods for Calculating Integrals of the Form (A.1)

A.5 Optimal Methods for Calculating Integrals of the Form (A.1)

A.5.1 Lower Bounds for the Functionals ? nm and ? N

In this section we derive lower bounds for the functionals ? nm and ? N, defined in Section A.2 , for calculating integrals (A.1) by the cubature formulas

(A.11)

and

(A.12)

on H lder and Sobolev classes.

Theorem A.5

Let ? = ( D) or ? = ( D), and calculate integral (A.1) by formula (A.11) with ? 1 = ? 2 = 0. Then the inequality


where , and

(A.13)

is valid.

Corollary A.2

Let ? = H ??( D) or , and calculate integral (A.1) by formula (A.11) with n 1 = n 2 = n and ? 1 = ? 2 = 0. Then the inequality


is valid.

Proof of Theorem A.5. Denote by ?( s 1, s 2) a nonnegative function belonging to the class (1) and vanishing at the nodes , 1 ? k 1 ? n 1, 1 ? k 2 ? n 2.

One has:

(A.14)

From Lemma A.5 and Theorem A.3 one concludes that the following inequality


holds for arbitrary weights and nodes and


Theorem A.5 is proved.

Theorem A.6

Let or , i = 1, 2, 3, and calculate the integral K f by cubature formula (A. 12). Then


where ,

UNLIMITED FREE
ACCESS
TO THE WORLD'S BEST IDEAS

SUBMIT
Already a GlobalSpec user? Log in.

This is embarrasing...

An error occurred while processing the form. Please try again in a few minutes.

Customize Your GlobalSpec Experience

Category: Digital-to-Analog Converters
Finish!
Privacy Policy

This is embarrasing...

An error occurred while processing the form. Please try again in a few minutes.