Total and Scattered Field Formulations in the Transfinite Element Method

2008 ◽  
Vol 44 (6) ◽  
pp. 778-781 ◽  
Author(s):  
I. Bardi ◽  
Z. Badics ◽  
Z.J. Cendes
2007 ◽  
Vol 43 (4) ◽  
pp. 1349-1352 ◽  
Author(s):  
C. Stockreiter ◽  
G. Matzenauer ◽  
O. Biro ◽  
P. Caldera ◽  
K. Preis ◽  
...  

Author(s):  
Phan Hai Dang ◽  
Le Duc Tho ◽  
Le Quang Hung ◽  
Dao Duy Kien

The current article is concerned with the interaction of Rayleigh waves with surface defects of arbitrary shape in a homogeneous, isotropic, linearly elastic half-space. Using a linear superposition principle, the interaction generates a scattered field which is equivalent to the field radiated from a distribution of horizontal and vertical tractions on the surface of the defect. These tractions are equal in magnitude but opposite in sign to the corresponding tractions obtained from the incident wave. The scattered field is then computed as the superposition of the displacements radiated from the tractions at every point of the defect surface using the reciprocity theorem approach. The far-field vertical displacements are compared with calculations obtained by the boundary element method (BEM) for circular, rectangular, triangular and arbitrary-shaped defects. Comparisons between the theoretical and BEM results, which are graphically displayed, are in excellent agreement. It is also discussed the limitations of the proposed approximate theory. Keywords: half-space; Rayleigh wave; surface defect; reciprocity theorem; boundary element method (BEM).


Author(s):  
Zhongwei Jin ◽  
ganghua qin ◽  
haidong fan ◽  
ruochen huang ◽  
ziqi chen ◽  
...  

The magnetic polarization tensor has a promising capability of determining the geometry and material properties of metallic samples. In this paper, a novel computation method is proposed to estimate the magnetic polarization tensors for the metallic samples using the boundary element method. In this method, the metallic sample is placed in a uniformly distributed magnetic field. Based on assumptions that the excitation frequency and/or the conductivity of the sample is very high, the metallic sample is regarded as a perfect electrical conductor (PEC). Therefore, the scattered field at a certain distance can be simulated. By utilising the boundary element method, the magnetic polarization tensor can be derived from the simulated scattered field. The theoretical calculation is presented and simulations and experiments have been carried out to validate the proposed method. The results from the simulation are matched with the analytical solution for the case of sphere samples. Moreover, there is a good agreement between the simulation results and the experimental results for the copper cylindrical samples.


2000 ◽  
Vol 36 (10) ◽  
pp. 881 ◽  
Author(s):  
Ning Yuan ◽  
A.J. Parfitt ◽  
J.S. Kot

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