区域地震事件的纵横波差异与震源类型

简要介绍地震与爆炸的震源物理性质及地震波激发机制特征。利用地震观测波形直达纵横波震相能量释放的差异,在时间域引进标志事件震源性质的参量a。132个台站记录的22个不同震源类型事件的计算结果表明,a值具有震源性质依附效应,展现出在事件识别领域的应用前景。     

基于电场不连续边界条件的层状介质电磁格林函数计算

给出了适用于全空间层状模型偶极子源格林函数的去奇异性广义描述技术。过源平行于层界面设置一个虚界面,使相邻层界面限制的区域中电磁矢量势函数可以分解为TE模式和TM模式标量势函的叠加,且它们都满足齐次Helmhlotz方程,相应的解可以通过叠加上行波和下行波函数得到。源的奇异性被耦合到切向电磁场所满足的不连续边界条件上,并通过反射系数所描述的振幅递推关系延拓到其他任意层中,实现了全空间任意位置格林函数的计算。该思路被应用到VED源激发的海洋电磁模型数值模拟中,计算结果很好地反映了电磁场在海洋模型中的传播过程,验证了该技术思路的正确性。     

The PWaves From the Amchitka Island Explosions

Summary. There is evidence that the equivalent seismic sources of the Amchitka Island explosions — Longshot, Milrow and Cannikin — depart significantly from the simple model of a point compressional-source in a layered elastic-medium. Consequently modelling the observed seismograms using standard source-models may not be the most efficient method of determining source properties. Here an alternative to modelling is used to obtain information on the seismic sources due to the explosions. Broad-band (BB) estimates of the P signals are obtained from the short-period (SP) seismograms, corrected for attenuation, and interpreted in terms of P, pP and radiation from secondary sources. the main conclusions are:
(i) BB estimates of the radiated displacement from the explosions can be obtained with only a small reduction in the signal-to-noise ratio seen on SP seismograms;
(ii) observations of differences in pulse amplitudes and spectra are not necessarily due to differences in anelastic attenuation;
(iii) P and pP at a given station may differ in shape so that notches in the signal spectrum may not be related to source depth;
(iv) there is evidence of arrivals that others have identified as due to slap-down but which could be interpreted as an overshoot to pP;
(v) direct interpretation of the estimated ground displacement is a better procedure for determining the seismic source properties of explosions than modelling SP seismograms using idealised models as a starting point.     

Features of Kamiokande-II,IMB, and Baksan observations and their interpretation in a two-component model for the signal

We consider the time, angular, and energy distributions of SN 1987A events and discuss the quality of their agreement with the expectations. A global interpretation is made by considering a simple model based on the standard scenario for the explosion. Despite the contrasting and confusing indications, a straightforward fit to the data provides a result that does not contradict but rather supports the expectations. The calculated electron antineutrino flux is applied to predict the relic neutrino signal. The article was translated by the authors.     

水泥土微观结构特征的定量评价

介绍了利用图像处理技术对土体进行微观结构定量分析方法,讨论了表征结构单元体和孔隙大小、形态及定向性等结构要素的定量评价指标。通过对加入水泥固化后软土的微观结构图像分析,论证了水泥土的微观结构特征定量分析方 法,得出了以此来分析评价土体微观结构特征的方法。     

Analysis of infrasonic and seismic events related to the 1998 Vulcanian eruption at Sakurajima

We present results from a detailed analysis of seismic and infrasonic data recorded over a four day period prior to the Vulcanian eruptive event at Sakurajima volcano on May 19, 1998. Nearly one hundred seismic and infrasonic events were recorded on at least one of the nine seismic–infrasonic stations located within 3 km of the crater. Four unique seismic event types are recognized based on the spectral features of seismograms, including weak seismic tremor characterized by a 5–6 Hz peak mode that later shifted to 4–5 Hz. Long-period events are characterized by a short-duration, wide spectral band signal with an emergent, high-frequency onset followed by a wave coda lasting 15–20 s and a fundamental mode of 4.2–4.4 Hz. Values of Q for long-period events range between 10 and 22 suggesting that a gas-rich fluid was involved. Explosive events are the third seismic type, characterized by a narrow spectral band signal with an impulsive high-frequency onset followed by a 20–30 second wave coda and a peak mode of 4.0–4.4 Hz. Volcano-tectonic earthquakes are the fourth seismic type. Prior to May 19, 1998, only the tremor and explosion seismic events are found to have an infrasonic component. Like seismic tremor, infrasonic tremor is typically observed as a weak background signal. Explosive infrasonic events were recorded 10–15 s after the explosive seismic events and with audible explosions prior to May 19. On May 19, high-frequency impulsive infrasonic events occurred sporadically and as swarms within hours of the eruption. These infrasonic events are observed to be coincident with swarms of long-period seismic events. Video coverage during the seismic–infrasonic experiment recorded intermittent releases of gases and ash during times when seismic and acoustic events were recorded. The sequence of seismic and infrasonic events is interpreted as representing a gas-rich fluid moving through a series of cracks and conduits beneath the active summit crater.