The Birth of Modern Seismology in the Nineteenth and Twentieth Centuries

2007 ◽  
Vol 26 (2) ◽  
pp. 263-280 ◽  
Author(s):  
Johannes Schweitzer

The earliest seismic instruments were seismoscopes, which could only indicate that a ground shaking had occurred. Modern seismology started in the late 19th century when, mostly in Italy, Japan, Russia, and Germany, seismic instruments were developed, which were able to record ground movements as function of time and orientation. During the decade before World War I, the fundamental development of seismic instruments was completed with seismograph systems of high resolution in time and enough sensitivity to record the most important seismic phases. Since seismic waves traverse the whole Earth and do not stop at political borders, the seismological discoveries were only possible after developing new structures for internationally organized data exchange and cooperation. In parallel to instrumental and organizational developments, seismologists had to learn the principles of seismic wave propagation in a solid body based on elasticity and ray theory. A stepwise deciphering of seismic wave speeds inside the Earth for the different seismic phase types led to the discovery of the basic structure of our planet consisting of crust, mantle and a core divided in two parts.

2020 ◽  
Vol 224 (2) ◽  
pp. 1443-1463
Author(s):  
Victor Mensah ◽  
Arturo Hidalgo

SUMMARY The accurate numerical modelling of 3-D seismic wave propagation is essential in understanding details to seismic wavefields which are, observed on regional and global scales on the Earth’s surface. The diffusive-viscous wave (DVW) equation was proposed to study the connection between fluid saturation and frequency dependence of reflections and to characterize the attenuation property of the seismic wave in a fluid-saturated medium. The attenuation of DVW is primarily described by the active attenuation parameters (AAP) in the equation. It is, therefore, imperative to acquire these parameters and to additionally specify the characteristics of the DVW. In this paper, quality factor, Q is used to obtain the AAP, and they are compared to those of the visco-acoustic wave. We further derive the 3-D numerical schemes based on a second order accurate finite-volume scheme with a second order Runge–Kutta approximation for the time discretization and a fourth order accurate finite-difference scheme with a fourth order Runge–Kutta approximation for the time discretization. We then simulate the propagation of seismic waves in a 3-D fluid-saturated medium based on the derived schemes. The numerical results indicate stronger attenuation when compared to the visco-acoustic case.


Geophysics ◽  
1937 ◽  
Vol 2 (4) ◽  
pp. 319-328 ◽  
Author(s):  
Morris Muskat

It is suggested that in the computation of theoretical time‐distance curves for seismic wave propagation a more tractable form of analysis is obtained if the depth is expressed as a power series in the velocity than when the converse but more conventional method is used. Several illustrations of this procedure are given.


1971 ◽  
Vol 61 (3) ◽  
pp. 697-706 ◽  
Author(s):  
Walter W. Hays ◽  
John R. Murphy

abstract Yucca Fault is a major structural feature of Yucca Flat, a well-known geological province of the Nevada Test Site (NTS). The trace of the Fault extends north-south over a distance of about 32 km. The fault plane is nearly vertical and offsets Quaternary alluvium, Tertiary volcanic tuffs and pre-Cenozoic basement rocks (quartzites, shales and dolomites) with relative down displacement of several hundred feet on the east side of the fault. Data recorded from the CUP underground nuclear detonation in Yucca Flat typify the effect of the fault on near-zone (i.e., inside 10 km) seismic wave propagation. The effect of the fault is frequency dependent. It affects the frequency components (3.0, 5.0, 10.0 Hz) of the seismic waves which have characteristic wavelengths in the order of the geological discontinuity. Little or no effect is observed for low-frequency components (0.5, 1.0 Hz) which have wave-lengths exceeding the dimensions of the geological discontinuity. The effect of the fault does not represent a safety problem.


2012 ◽  
Vol 11 (2) ◽  
pp. 594-609 ◽  
Author(s):  
S. Chaillat ◽  
J.F. Semblat ◽  
M. Bonnet

AbstractThe analysis of seismic wave propagation and amplification in complex geological structures requires efficient numerical methods. In this article, following up on recent studies devoted to the formulation, implementation and evaluation of 3-D single- and multi-region elastodynamic fast multipole boundary element methods (FM-BEMs), a simple preconditioning strategy is proposed. Its efficiency is demonstrated on both the single- and multi-region versions using benchmark examples (scattering of plane waves by canyons and basins). Finally, the preconditioned FM-BEM is applied to the scattering of plane seismic waves in an actual configuration (alpine basin of Grenoble, France), for which the high velocity contrast is seen to significantly affect the overall efficiency of the multi-region FM-BEM.


2017 ◽  
Vol 56 (1) ◽  
Author(s):  
Román Álvarez

Mexico City experienced a large amount of damage during the September 19, 1985, earthquake. Although the whole city experienced different destruction degrees the region of maximum damage was constrained to a densely populated area west from the international airport, where water saturated sediments are still abundant. Other regions within the city, also with saturated sediments, did not experience a similar destruction. Among the mechanisms proposed to explain such large amount of destruction, one was proposed involving the interaction of incoming and reflected seismic waves in, or close to, the saturated surface. The existence and location of seismic wave reflecting surfaces within the basin of Mexico is thus of basic importance. It is herein proposed that high-density geologic structures within the basin may constitute those reflecting surfaces. 2-D gravity modeling is performed across the basin between Sierra del Tepeyac(N) and Xochimilco (S); some lines intersect and model volcanic structures in this region. A 3-D inversion of the gravity field shows that Sierra del Tepeyac-Peñón de Los Baños is a dense structure potentially capable of reflecting seismic waves towards the west, while Sierra de Santa Catarina would preferentially reflect them towards the south. The high-density regions are defined and mapped in 3-D space. These findings support the possibility of strong interactions between seismic waves travelling in opposite directions in selected regions of the Mexico basin. The reflection mechanism will obviously be proportional to the magnitude of the originating seismic disturbance.


2021 ◽  
Vol 249 ◽  
pp. 13001
Author(s):  
Paul Sánchez ◽  
Daniel J. Scheeres

Through numerical simulations, we investigate impact generated seismic wave transmission in granular media under extremely low pressure. This mimics the conditions in the interior of asteroids and other small planetary bodies. We find a dependency not only on the overburden pressure on the medium, but also on the velocity of the impact that generates the wave. This is, at extremely low values of overburden pressure, the wave speed depends no only on the imposed pressure, but also on the increment in pressure created by the passing of the wave. We study crystalline and random packings and find very similar behaviour though with different wave speeds as expected. We then relate our results to different mission-related events on asteroids.


2020 ◽  
Vol 117 (47) ◽  
pp. 29504-29511
Author(s):  
Lucia Gualtieri ◽  
Etienne Bachmann ◽  
Frederik J. Simons ◽  
Jeroen Tromp

The interaction of ocean surface waves produces pressure fluctuations at the seafloor capable of generating seismic waves in the solid Earth. The accepted mechanism satisfactorily explains secondary microseisms of the Rayleigh type, but it does not justify the presence of transversely polarized Love waves, nevertheless widely observed. An explanation for two-thirds of the worldwide ambient wave field has been wanting for over a century. Using numerical simulations of global-scale seismic wave propagation at unprecedented high frequency, here we explain the origin of secondary microseism Love waves. A small fraction of those is generated by boundary force-splitting at bathymetric inclines, but the majority is generated by the interaction of the seismic wave field with three-dimensional heterogeneity within the Earth. We present evidence for an ergodic model that explains observed seismic wave partitioning, a requirement for full-wave field ambient-noise tomography to account for realistic source distributions.


Sign in / Sign up

Export Citation Format

Share Document