Behaviour of Electromagnetic Waves in Different Media and by Edited by: Ali Akdagli PDF

By Edited by: Ali Akdagli

ISBN-10: 9533073020

ISBN-13: 9789533073026

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S. (1993-1994). Roughness of smooth surfaces: STM versus profilometers. Metro-logia 30. 513-516. [15] Stedman, M. (1992). The performance and limits of scanning probe microscopes. In Proc. Int. Congr. X-ray Optics and Microanalysis, pp. 347-352, Manchester. IOP Publishing Ltd. V. V. (1980). On the Weirstrass-Mandelbrot fractal function. Royal Soc. 459. 0 3 Electromagnetic Wave Scattering from Material Objects Using Hybrid Methods Adam Kusiek, Rafal Lech and Jerzy Mazur Gdansk University of Technology, Faculty of Electronics, Telecommunications and Informatics Poland 1.

Scattered field from the previous iteration coming from K − 1 objects is assumed to be a new inc (1) incident field Fi on ith object in first iteration (see Fig. 5) and is defined as follows: inc (1) Fi inc (0) where: Fij = K inc (0) ∑ Fij , (1) j =1 j =i is a scattered field from jth object in zero iteration transformed to local scat(1) coordinates xi yi zi . Once again we derive the scattered field Fi for each ith object in the configuration. During the iteration process the scattered field from the previous iteration (from K-1 posts) is utilized as a new incident field on the remaining post and the coefficients of the pth iteration depend only on the coefficients of the (p − 1)th iteration.

The phases ϕnm can be chosen determinedly or casually, receiving accordingly determine or stochastic function z ( x , y ) . We further shall consider ϕnm as casual values, which in regular distributed on a piece −π ; π . With each particular choice of numerical meanings all N × M phases ϕnm (for example, with the help of the generator of random numbers) we receive particular (with the beforehand chosen meanings of parameters c w , q , K , D, N , M ) realization of function z ( x , y ) . The every possible realizations of function z ( x , y ) form ensemble of surfaces.

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