Parallel Hybrid Algorithm for Three-Dimensional Elastic Wave Scattering in Steel Pipes

2004 ◽  
Vol 126 (4) ◽  
pp. 510-517 ◽  
Author(s):  
A. Mahmoud ◽  
A. H. Shah ◽  
N. Popplewell

A parallel computational algorithm that models three-dimensional elastic wave scattering in an infinite pipe is introduced. The algorithm combines two procedures: a Wave Function Expansion (WFE) and a Finite Element Discretization (FED). The WFE represents a flawless unbounded region while the FED idealizes a bounded region containing the defects. Unknown amplitudes in the WFE are determined by imposing continuity between the two regions; they are then used to calculate the reflection and transmission coefficients. The inversion of a large stiffness matrix resulting from the FED has been overcome in the current formulation by sub-structuring the finite element mesh. The algorithm is implemented in Fortran 90™ on a shared-memory, parallel computing platform using OpenMP™ directives. The algorithm is validated against available numerical and experimental results. Agreement with previous three-dimensional results for a radial crack in a steel pipe and a two-dimensional hybrid model of an axisymmetric cracked, welded steel pipe are shown to be excellent. New results are presented for an inclined crack in a steel pipe as well as for a non-axisymmetric cracked welded steel pipe.

1984 ◽  
Vol 51 (3) ◽  
pp. 614-621 ◽  
Author(s):  
J. H. Su ◽  
V. V. Varadan ◽  
V. K. Varadan

A finite element eigenfunction method (FEEM) is formulated for elastic wave scattering by bounded three-dimensional axisymmetric regions (cavity, homogeneous, or inhomogeneous) for harmonic waves incident at arbitrary angles. The solutions are hence three-dimensional and no longer axisymmetric. The scattering region is enclosed within a sphere. The scattered field outside the sphere is expanded in outgoing vector spherical functions. Within the sphere, basis-functions are generated by a finite element technique applying the vector spherical harmonics as boundary conditions. The field inside the sphere is then written as a superposition of these basis functions with unknown coefficients which are then solved by matching with the exterior field. Numerical results are obtained for a variety of scatterers and comparisons made with available results.


2003 ◽  
Vol 113 (6) ◽  
pp. 3012 ◽  
Author(s):  
Seiji Nakagawa ◽  
Kurt T. Nihei ◽  
Larry R. Myer ◽  
Ernest L. Majer

2018 ◽  
Vol 144 (4) ◽  
pp. EL268-EL274
Author(s):  
Zhen Li ◽  
Yuanda Su ◽  
Xiaoming Tang ◽  
Huanran Li ◽  
Qing Huo Liu

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