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Recovery of rough surface in ducting medium from grazing ...
www.damtp.cam.ac.uk/user/ms100/PAPERS/main-JAP.pdf13 Dec 2018: h(Xn) = z |Sn(xn Xn)3/2. αφ(Xn)δ|. (24). 2. Medium with Linear Profile. ... Reconstruct the surface h(Xn) by eq. (24) for uniformmedium or (26) for linear profile using Φ obtained aboveend for. -
doi:10.1016/j.ecss.2007.09.029
www.damtp.cam.ac.uk/user/ms100/PAPERS/Karunarathna_et_al_2008.pdf13 Dec 2018: The estuary receives water from a catchment coveringan area of 24,000 km2 and is the largest freshwater supplier to theNorth Sea. ... 0.0. 5.0. 10.0. 15.0. x (km. ). y (km) -30-28-26-24-22-20-18-16-14-12-10-8-6-4-20. 1925 1936. -
Recovery of a Variable Coefficient in a Coastal Evolution Equation
www.damtp.cam.ac.uk/user/ms100/PAPERS/JCP99.pdf13 Dec 2018: F′n1, An,n =τ. 2ξF′n. (24). This is easily and rapidly inverted by back-substitution. -
Sound propagation in an irregular two-dimensional waveguideMark…
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA97.pdf13 Dec 2018: and7!:. cr! 5 ESFG r;r8! ]c]z r8!2 ]G]z r;r8!cr8!Gdx8,. 24! where againr85[x8,S(x8)], and S is the union of the sur-facesh1 -
Coherent Field and Specular Reflection At Grazing Incidence on a…
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA94spec.pdf13 Dec 2018: 0 Zl ( (•(x,zi))=--• Do(X)-- likzi cos 0 --• COS 2 0 eikXx+ h(x)• ,. (24). where • is the variance of the surface height. Here we have neglected an O(a ... 29) Collecting terms, and using (25), (26), and (29), Eq. (24) can now be written. ( {• -
Numerical Solution of Scattering From a Hard Surface in a Medium with …
www.damtp.cam.ac.uk/user/ms100/PAPERS/JASA93.pdf13 Dec 2018: T-•=Tg'(1--To •AT Tg:A •. ) (24) so that. E = (2 - 4At 8A•. ... 2. It is easy and computationally inexpensive to take further terms in the se- ries (24). -
Rough surface backscatter and statistics via extended parabolic…
www.damtp.cam.ac.uk/user/ms100/PAPERS/arXiv1408.1879.pdf13 Dec 2018: By (24),〈h(X). I(r). r. 〉=. 〈h(X). d. dr. r0. ikh(r′) cos θeikSr. ′. ... 24] P. Tran, Calculation of the scattering of electromagnetic waves from a two-dimensional per-fectly conducting surface using the method of ordered multiple interaction, -
Efficient boundary integral solution for acoustic wave scattering by…
www.damtp.cam.ac.uk/user/ms100/PAPERS/arxiv1407.5560v1.pdf13 Dec 2018: elements. (Bn)mj = Anmnj. (24). We thus require. bn = B1n cn (25). ... from rough surfaces, Waves in Random Media, 6, 151-167 (1996). [24] A.A. -
PII: 0893-9659(90)90021-3
www.damtp.cam.ac.uk/user/ms100/PAPERS/AppMathLett90.pdf13 Dec 2018: g = (A’ B’)m. where. A’ = a2 -@g. 8’ = -2r [l -! Jtt, $1,! (<, 59 = f(E) f(d. l = @1- 22 - 23 td)/SL, 7 = (21 - 22 2s - 24)/2L, and -
Efficient boundary integral solution for acousticwave scattering by…
www.damtp.cam.ac.uk/user/ms100/PAPERS/acoust3d_eabe_b.pdf13 Dec 2018: 2.1. Formal solution and splitting series. The method of solution is analogous to that applied to the electromagneticproblem in 2-d or 3-d [23, 24]. ... 24] M. Spivack, J. Ogilvy, C. Sillence, Electromagnetic scattering by large com-plex scatterers in 3d,
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