Modeling of earthquake source parameters on December 12, 2018 (08:49:56,16; 36,4478° N; 140,5788° E; H = 62,0 km; Mw = 4,3, Japan)

IF 0.5 Q4 GEOCHEMISTRY & GEOPHYSICS
R.M. Pak, O. Hrytsai
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引用次数: 0

Abstract

Modeling of earthquake source parameters, such as the orientation of the fault plane and the direction of the fault slip, is important for understanding the physics of earthquake source processes, determining the stress-strain state of the geological medium and seismic hazard estimation. For modeling source parameters of the earthquake on December 12, 2018 at 08:49:56,16 (UTC) in Japan (36,4478° N, 140,5788° E, Northern Ibaraki Pref region) at a depth of 62 km with a magnitude of Mw = 4.3, the waveforms inversion was used to determine seismic moment tensor and representation it through a focal mechanism. The earthquake source is considered as a point source of seismic waves which propagate in a medium represented by a set of horizontally homogeneous elastic layers. An algorithm for determining seismic tensor components based on the forward problem solved by the matrix method, and using the generalized inverse solution, selecting only direct waves is applied. The input data for determining seismic moment components are data of only direct P waves selected from the observed records at six seismic stations of the Japanese local network NIED F-net: TSK, YMZ, ASI, ONS, SBT, KSK. The seismic moment tensor components were determined through waveform inversion using the matrix method. The obtained results, presented through a focal mechanism, are compared to the results obtained by the National Research Institute of Earth Sciences and Resistance to Natural Disasters (NIED CMT solutions). As a result of focal mechanisms comparison, it is concluded that the proposed algorithm for determining seismic moment tensor components can be used if it is impossible to use another method, or requires some refinement for another method. This approach is especially relevant for regions with low seismicity and insufficient number of stations. In addition, this method reduces the effects of an inaccurate medium model, because direct waves are much less distorted than reflected and converted, and that increases the accuracy and reliability of the method.
2018年12月12日(08:49:56,16)震源参数建模;36、4478°N;140年,5788°E;H = 62,0 km;Mw = 4,3(日本)
震源参数的建模,如断层面的方向和断层滑动的方向,对于理解震源过程的物理性质、确定地质介质的应力-应变状态和地震危险性估计非常重要。为了模拟2018年12月12日08:49:56,16(UTC)日本(364478°N,1405788°E,茨城县北部地区)62公里深处Mw=4.3级地震的震源参数,使用波形反演来确定地震矩张量,并通过震源机制表示。震源被认为是在由一组水平均匀弹性层表示的介质中传播的地震波的点源。基于矩阵法求解的正演问题,并使用广义逆解,仅选择直达波,应用了一种确定地震张量分量的算法。用于确定地震矩分量的输入数据是仅从日本本地网络NIED F-net的六个地震台站的观测记录中选择的直接P波的数据:TSK、YMZ、ASI、ONS、SBT、KSK。采用矩阵法通过波形反演确定了地震矩张量分量。将通过焦点机制得出的结果与国家地球科学和自然灾害抵抗研究所(NIED CMT解决方案)得出的结果进行了比较。作为震源机制比较的结果,得出的结论是,如果不可能使用另一种方法,或者需要对其他方法进行一些改进,则可以使用所提出的确定地震矩张量分量的算法。这种方法尤其适用于地震活动性低和台站数量不足的地区。此外,这种方法减少了不准确介质模型的影响,因为直接波比反射波和转换波失真小得多,这提高了该方法的准确性和可靠性。
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来源期刊
Geofizicheskiy Zhurnal-Geophysical Journal
Geofizicheskiy Zhurnal-Geophysical Journal GEOCHEMISTRY & GEOPHYSICS-
自引率
60.00%
发文量
50
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