Travel time distributions under convergent radial flow in heterogeneous formations: Insight from the analytical solution of a stratified model

2013 ◽  
Vol 60 ◽  
pp. 100-109 ◽  
Author(s):  
Daniele Pedretti ◽  
Aldo Fiori
2019 ◽  
Vol 206 ◽  
pp. 630-640 ◽  
Author(s):  
Xiaolong Li ◽  
Lianbang Wang ◽  
Meimei Hao ◽  
Yanhui Zhong ◽  
Bei Zhang

2015 ◽  
pp. 1-13
Author(s):  
H.-Y. Wang ◽  
X.-W. Tang ◽  
Y. Wang ◽  
Q. Tang ◽  
P.-L. Gan

2019 ◽  
Vol 489 (1) ◽  
pp. 84-88
Author(s):  
A. G. Fatyanov ◽  
V. Yu. Burmin

It is generally accepted that PKP‑waves precursors, which are observed on a real data ahead of PKP‑waves, are explained by scattering on small-scale inhomogeneities in the lower mantle. In this paper, a stable analytical solution (without interference) was obtained for the wave field of longitudinal waves in a layered (discrete) ball of planetary size. The calculations of the total wave field, rays and travel-time curves of longitudinal waves for the spherical model of the Earth AK135 with a carrier frequency of 1 hertz are presented. The analytical solution showed that at angles smaller than 145 degrees ahead of the PKP‑waves, low-amplitude waves appear, with a higher frequency of about 1,3 hertz. Indeed, these high-frequency oscillations have the form characteristic for waves scattered at a certain object. The ray pattern and the travel-time graph show that these high-frequency oscillations are due to exclusively to the spherical geometry of the Earth. This could be explained by the interference of refracted and reflected longitudinal waves in the bottom of a discrete outer core. This field propagates even further towards smaller angles due to the interference of diffraction waves.


2016 ◽  
Vol 23 (1) ◽  
pp. 23-35 ◽  
Author(s):  
H.-Y. Wang ◽  
X.-W. Tang ◽  
Q. Tang ◽  
Y. Wang ◽  
P.-L. Gan

2020 ◽  
Vol 8 (2) ◽  
pp. 21-25
Author(s):  
Olga Burtseva ◽  
Viktor Kochanenko ◽  
Sergej Evtushenko ◽  
Anatoly Kondratenko

The equations of motion of a non-stationary radial flow are derived, the boundary value problem is set, and its analytical solution is obtained. The solution of the problem in this paper is in good agreement with the experimental parameters obtained at the experimental setup for small perturbations. The equations for determining the height of the wave front that decreases downstream of the flow are obtained, and the instantaneous velocity of the wave front tends to zero.


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