Acoustic and Electromagnetic Scattering Analysis Using - download pdf or read online

Acoustic and Electromagnetic Scattering Analysis Using - download pdf or read online

By Adrian Doicu

ISBN-10: 0122197402

ISBN-13: 9780122197406

The discrete resources process is an effective and strong device for fixing a wide category of boundary-value difficulties in scattering idea. a number of numerical equipment for discrete assets now exist. during this ebook, the authors unify those formulations within the context of the so-called discrete assets strategy. Key beneficial properties* accomplished presentation of the discrete assets procedure* unique concept - an extension of the traditional null-field technique utilizing discrete resources* useful examples that reveal the potency and suppleness of elaborated equipment (scattering through debris with excessive element ratio, tough debris, nonaxisymmetric debris, a number of scattering)* record of discrete resources programmes to be had through the net

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Additional info for Acoustic and Electromagnetic Scattering Analysis Using Discrete Sources

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12: Consider Di a bounded domain of class C^. Let the set { x ~ } ^ i be dense on a surface S" enclosed in Di and let the set 54 CHAPTER III SYSTEMS OF FUNCTIONS IN ACOUSTICS { ^ n l ^ i ^^ dense on a surface 5"^ enclosing Di. Then each of the systems (a) {t/;;,n = l , 2 , . . / Im(fcA) > 0, fc ^ p ( A ) } is complete in L'^{S). Proof: Let us consider (a). 49) where Ua' is the single-layer potential with density a' = a*. By a density argument it follows that du / t^a'-fA-^ = 0 o n 5 - . 50) Application of the first Green theorem in the region D~ yields ^ d 5 = Im(fc) /" (|fc|2 | t i „ f + \Vua-f) s- AV.

4 we can state the following result. 8: Consider the bounded sequence (zn) C F^, where Fz is a segment of the z-axis. ,m G Z. Then, the resulting systems of functions are complete in L'^{S). Proof: For proving the first part of the theorem it suffices to establish the explicit form of the vanishing conditions l i m 2 ^ ( ^ ) / ( M ' ' " ' = ^ ( . ^ n ) = 0,n = l , 2 , . . , m e Z . 40) Using the representation (cf. (i 4 H ) ! 2 ^ ' + I " ' I (fe^)"^"''""" J2iMmm). 41) where Sm are the ring currents corresponding to x?

Since u is an analytic function we deduce that u = 0 in any bounded domain of R^. Choose now a spherical surface S^ enclosing S. Clearly, w = 0 on 5 ^ and we may use the addition theorem for regular spherical wave function ^J„„(x) = u i . "'(-^") m=—TTimax n'>|m| \ n = l "mn'(x) = 0 . , x € 5 « . ,mmax, n' > |m|. 85) n=l Multiplying the above equation by u^^, (x), where x G -Df and D f is the exterior of 5^, summing over m and n' and accounting for the addition theorem for radiating spherical wave functions we arrive at (•max E "-max E "'n"4n(x) = 0, X € Df.

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Acoustic and Electromagnetic Scattering Analysis Using Discrete Sources by Adrian Doicu


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