scholarly journals Analysis of a finite PML approximation to the three dimensional elastic wave scattering problem

2010 ◽  
Vol 79 (272) ◽  
pp. 2079-2079 ◽  
Author(s):  
James H. Bramble ◽  
Joseph E. Pasciak ◽  
Dimitar Trenev
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

1990 ◽  
Vol 43 (10) ◽  
pp. 235-249 ◽  
Author(s):  
Herbert U¨berall ◽  
P. P. Delsanto ◽  
J. D. Alemar ◽  
E. Rosario ◽  
Anton Nagl

The singularity expansion method (SEM), established originally for electromagnetic-wave scattering by Carl Baum (Proc. IEEE 64, 1976, 1598), has later been applied also to acoustic scattering (H U¨berall, G C Gaunaurd, and J D Murphy, J Acoust Soc Am 72, 1982, 1014). In the present paper, we describe further applications of this method of analysis to the scattering of elastic waves from cavities or inclusions in solids. We first analyze the resonances that appear in the elastic-wave scattering amplitude, when plotted vs frequency, for evacuated or fluid-filled cylindrical and spherical cavities or for solid inclusions. These resonances are interpreted as being due to the phase matching, ie, the formation of standing waves, of surface waves that encircle the obstacle. The resonances are then traced to the existence of poles of the scattering amplitude in the fourth quadrant of the complex frequency plane, thus establishing the relation with the SEM. The usefulness of these concepts lies in their applicability for solving the inverse scattering problem, which is the central problem of NDE. Since for the case of inclusions, or of cavities with fluid fillers, the scattering of elastic waves gives rise to very prominent resonances in the scattering amplitude, it will be of advantage to analyze these with the help of the resonance scattering theory or RST (first formulated by L Flax, L R Dragonette, and H U¨berall, J Acoust Soc Am 63, 1978, 723). These resonances are caused by the proximity of the SEM poles to the real frequency axis, on which the frequencies of physical measurements are located. A brief history of the establishment of the RST is included here immediately following the Introduction.


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