Finite Difference Modeling of T-phase Propagation from Ocean to Land
نویسندگان
چکیده
We model the T-Phase transition from ocean to land and evolution of the seismic signal through this process. We model the transition with a composite technique using normal mode based numerical propagation codes to calculate the hydroacoustic pressure field in the ocean, and use this pressure field as input for the elastic finite difference code TRES to calculate the seismic propagation to land-based stations. Animations are created from the finite difference calculations to help visualize the complex conversion process. We have performed a detailed study of the transition from the Point Sur interim IMS station to seismic stations along the California coast. The numerical calculations performed to date are accurate to 9 Hz. An unusual result of the analysis that is observed both in the data and the calculations is that converted surface waves arrive at coastal stations earlier than body waves. This occurs because conversion to surface waves occurs farther offshore than conversion to body waves. For a typical coastal structure, the P-waves arrive in the middle of the surface wavetrain and are obscured at stations near the coast. T-phases propagate primarily as P-waves once they are well inland from the coast and the surface waves have been attenuated. We have performed a number of test cases to assess the robustness of these results. Calculations for slopes varying from 10 degrees to 30 degrees show little difference in the results. Other studies have reported stronger effects for steeper slopes. All of the IMS T-Phase stations, however, are located in areas where the offshore slope is less than 30 degrees. The California calculations have a low velocity surface layer, so we performed a set of calculations with the ocean embedded in a uniform structure. Again, the results are similar with coastal waveforms dominated by surface waves. In a faster, more uniform structure, however, the P-wave may appear ahead of the surface wave for slopes of 30 degrees or higher. We are continuing this research by performing calculations for paths to the IMS T-Phase stations, using the bathymetry along selected paths to those stations. OBJECTIVE The objective of this project is to better understand the propagation of T-phases from ocean to land, and the performance of T-phase International Monitoring System (IMS) stations, through empirical and numerical methods. The empirical study uses data from pressure sensors in the ocean and coastal and island seismometers to examine the T-phase transfer function. The numerical study uses finite difference calculations to model propagation of Tphases from ocean to land. RESEARCH ACCOMPLISHED The International Monitoring System (IMS) hydroacoustic network is a relatively sparse network consisting of 6 underwater hydroacoustic stations and 5 land-based seismic T-phase stations as shown in Figure 1. The hydroacoustic stations are much more sensitive to underwater signals than the T-phase stations and have a higher sampling rate and broader frequency range. The broader frequency range is important for identifying explosions, which are characterized by higher frequency content than other sources. Because of these limitations of T-phase stations, it is important to understand the efficiency of T-phase conversion in order to assess the capabilities of the IMS network for detection and identification of underwater sources. We are in the third year of a three year project to investigate these issues. In our presentations over the past two years, we described the following research: Report Documentation Page Form Approved
منابع مشابه
Three-dimensional Modeling of the Hydroacoustic to Seismic T-phase Transition
Plans call for five T-phase stations to be installed as part of hydroacoustic segment of the International Monitoring System (IMS), for use in detecting nuclear explosions in the oceans. The ability to detect T-phase signals at the seismic T-phase stations relies on an understanding of the transition from ocean-borne acoustic energy to seismic energy. Observations of the seismic T-phase indicat...
متن کاملImpact of Ocean-Land Mixed Propagation Path on Equivalent Circuit of Grounding Rods
In this paper, the effect of ocean-land mixed propagation path on the lightning performance of grounding rods is investigated. This effect is focused on two problems. The first is extracting exact equivalent circuit of grounding rods in the presence of oceans. The equivalent circuit can be used in transient analysis of power systems in the neighboring oceans. In the second one, this effect on t...
متن کاملMPI- and CUDA- implementations of modal finite difference method for P-SV wave propagation modeling
Among different discretization approaches, Finite Difference Method (FDM) is widely used for acoustic and elastic full-wave form modeling. An inevitable deficit of the technique, however, is its sever requirement to computational resources. A promising solution is parallelization, where the problem is broken into several segments, and the calculations are distributed over different processors. ...
متن کاملFinite-Difference Time-Domain Simulation of Light Propagation in 2D Periodic and Quasi-Periodic Photonic Structures
Ultra-short pulse is a promising technology for achieving ultra-high data rate transmission which is required to follow the increased demand of data transport over an optical communication system. Therefore, the propagation of such type of pulses and the effects that it may suffer during its transmission through an optical waveguide has received a great deal of attention in the recent years. We...
متن کاملSeismic Wave-Field Propagation Modelling using the Euler Method
Wave-field extrapolation based on solving the wave equation is an important step in seismic modeling and needs a high level of accuracy. It has been implemented through a various numerical methods such as finite difference method as the most popular and conventional one. Moreover, the main drawbacks of the finite difference method are the low level of accuracy and the numerical dispersion for l...
متن کامل