scholarly journals Hybrid of surface shear waves at the contact interface between piezoelectric and electrically conductive half-spaces

2021 ◽  
Vol 74 (3) ◽  
pp. 53-61
Author(s):  
A.S. Avetisyan ◽  
A.V. Gevorgyan ◽  
L.V. Avetisyan
1987 ◽  
Vol 23 (3) ◽  
pp. 207-211
Author(s):  
V. V. Levchenko ◽  
N. A. Shul'ga

1976 ◽  
Vol 102 (3) ◽  
pp. 413-414
Author(s):  
D. Howell Peregrine
Keyword(s):  

1979 ◽  
Vol 70 (2) ◽  
pp. 375-382 ◽  
Author(s):  
J.A de Feijter ◽  
J Benjamins
Keyword(s):  

1975 ◽  
Vol 101 (7) ◽  
pp. 1032-1034
Author(s):  
Edward H. Wilson
Keyword(s):  

1974 ◽  
Vol 100 (9) ◽  
pp. 1215-1227
Author(s):  
D. Howell Peregrine
Keyword(s):  

2019 ◽  
Vol 184 (1) ◽  
pp. 21-42 ◽  
Author(s):  
Andrey Sarychev ◽  
Alexander Shuvalov ◽  
Marco Spadini

Complexity ◽  
2021 ◽  
Vol 2021 ◽  
pp. 1-12
Author(s):  
Uma Bharti ◽  
Pramod Kumar Vaishnav ◽  
S.M. Abo-Dahab ◽  
Jamel Bouslimi ◽  
K.H. Mahmoud

Irregularity may occur on the earth’s surface in the form of mountains due to the imperfection of the earth’s crust. To explore the influence of horizontally polarized shear waves on mountains, we considered the fluid-saturated porous medium (superficial layer) over an orthotropic semi-infinite medium with rigid (Model-I) and soft (Model-II) mountain surfaces for wave propagation. The mountain surface is defined mathematically as a periodic function of the time domain. The physical interpretation of materials’ structure has been explained in rectangular Cartesian coordinate system originated at the contact interface of layer and half-space. The displacement of the mountains has been derived by solving energy equations analytically. The influence of rigid and soft mountain surfaces on the phase velocity of shear waves has been demonstrated graphically (we used MATLAB software for graphical representations).


1999 ◽  
Vol 10 (5) ◽  
pp. 381-389
Author(s):  
Manidipa Chattopadhyay ◽  
S.K. Chakraborty ◽  
Sarbani Chakraborty

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