scholarly journals MODELING OF DISTRIBUTION OF SOUND WAVES IN THE CLOSED AREA BY FINITE DIFFERENCE METHOD

Akustika ◽  
2019 ◽  
Vol 32 ◽  
pp. 115-119
Author(s):  
Vladimir Mondrus ◽  
Dmitrii Sizov

The article contains a solution to the problem of wave propagation from two sources in the form of pulsating spheres located in a closed region asymmetrically about its boundary. The solution is produced by the explicit Euler method and the predictor-corrector method. Various types of boundary conditions are considered, including taking into account the “sticking” of the transfer medium to the walls of the closed region and in the form of an absolutely rigid wall, when only the normal velocity component is zero. Isopole potentials are given, as well as velocities and pressures at different points in time. The text of the article contains an analysis of the effect of the steps in time and coordinates on the results of the calculation.

Geophysics ◽  
1996 ◽  
Vol 61 (4) ◽  
pp. 1230-1231 ◽  
Author(s):  
Boris Gurevich

In their interesting paper the authors present a new advanced approach to the simulation of seismic wave propagation in media described by Biot’s theory of dynamic poroelasticity in two dimensions. The algorithm developed can be used to accurately simulate the effect of dynamic poroelasticity on seismic wavefields over hydrocarbon reservoirs. In cases where this effect proves significant this algorithm can be incorporated in the seismic modeling technology.


Geophysics ◽  
1984 ◽  
Vol 49 (9) ◽  
pp. 1457-1465 ◽  
Author(s):  
M. A. Dablain

The significance of entropy‐like terms is examined within the context of the finite‐difference modeling of acoustic wave propagation. The numerical implications of dissipative mechanisms are tested for performance within two very distinct differencing algorithms. The two schemes which are reviewed with and without dissipation are (1) the standard central‐difference scheme, and (2) the Lax‐Wendroff two‐step scheme. Numerical results are presented comparing the short‐wavelength response of these schemes. In order to achieve this response, the linearized version of an exploding one‐dimensional source is used.


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