模拟倾斜界面情况下区域地震范围内的长周期Pnl波          下载免费PDF全文

曹柏如  谢小碧 《地球物理学报》1992,35(2):185-192

中国大陆地壳厚度的特点是东部地区薄西部地区厚,因此在计算Pnl波的Green函数时进一步考虑了莫霍界面倾斜的影响.本文将广义射线理论推广到倾斜层结构模型,该方法的计算结果与有限差分的计算结果有很好的一致性.理论计算表明,在同一个倾斜结构模型中沿相反方向传播的Pnl波有明显的差异.因此当地壳厚度的变化不能忽略时,根据水平层模型的理论计算结果拟合Pnl波记录时效果不够理想.对菏泽、门源地震资料的处理结果表明,用一个更接近实际地壳的倾斜层模型来拟合Pnl波比用等效厚度平行层模型来拟合要更为合理.  相似文献   

电离层诸参量对大气重力波的响应与重力波参数反演          下载免费PDF全文

Schle.  K 马淑英 《地球物理学报》1992,35(4):405-414

本文利用欧洲非相干散射雷达数据,分析研究了电离层不同等离子体参量对大气重力波的响应之间的关系.应用这种关系,发展了一种在垂直于地磁场的电场可以忽略等简化假设下,由电子密度和离子沿场速度的同时测量数据,反演求解较高（约250km以上）F区中引起TID的重力波传播参数的方法.用此法对一典型TID事件进行分析计算,所得结果与全波解数值研究结果很好符合.  相似文献   

初动在核爆监测中的应用及分析     

张永荣 《地震地磁观测与研究》1992,13(1):24-30

核爆炸与地震相比,围绕爆炸源的初动具有更多的向上记录和更高的振幅周期比,初动可以作为核爆与地震的一个识别标志。某些核爆炸的向下记录。或许是由于低信噪比的原因,记录到的是初至波的第二个半周;其余的也许是由于近P波走时曲线的反射波造成。  相似文献   

核面反射波ScP在短周期仪器上的记录特征     

唐燕娟  寿海涛 《地震地磁观测与研究》1992,13(1):31-33

核面反射波ScP在短周期仪器垂直分量上有清楚记录,佘山台在DD-1仪器上,P和ScP记录的到时差为T_(SOP-P)=6~m±30.0~9左右。在此范围内震源深度不同,震中距差别也较大,从△=26°到40°左右。它的周期与P波相似,震源深度越深,ScP震相越尖锐,地动位移比(ScP/P)也相对越大。初分者有可能错分为另一次地震的P波,发生在海洋地区的地震记录ScP震相比较多。  相似文献   

泰安地区近震波速及地壳厚度的测定     

刘洪瑞  肖凤莲 《地震地磁观测与研究》1992,13(4):25-29

本文第一部分选取泰安台473型地震仪1985—1990年记录的70个地震资料,通过计算,得到泰安台附近的地壳厚度为H=36.5km,直达波的平均传播速度:V_P=6.18km/s、V_s=3.55km/s;反射波的传播速度:V_(P11)=6.45km/s、V_(S11)=3.79km/s;绕射波的传播速度:V_(Pn)=7.95km/s;平均虚波速度:V_φ=8.34km/s;平均波速比K=1.74。第二部分选取了泰安台基式地震仪有SP′震相记录的地震21个,求出了泰安台附近的地壳厚度为37km,并分析了SP′震相在泰安台的记录特征,初步得到SP′震相可观测范围为25°—60°。  相似文献   

均匀离散分布的平面应变过程和Fry法应变测量     

杨新岳 《大地构造与成矿学》1993,17(1):82-92

本文运用 Apple Macitonsh 计算机对无应变的均匀离散点分布进行系列平面应变模拟,应变叠加模式分别采用具普遍意义的成岩压实+顺层缩短(LPS)+压溶作用和成岩压实+简单剪切+压溶作用。对各应变阶段的变形点分布进行相应的 Fry 法应变测量,并配合低变形砂岩样品的 Fry 法应变分析实例.证实 Fry 法应变测量方法为一非常有用的应变测量方法,其结果不仅能较好地揭示全岩总应变特征,而且能揭示出许多应变叠加的信息,Fry 法揭示的全岩有限应变椭球主面的方位也较为真实可靠。而 Fry 法运用于应变分布不均匀的劈理化岩石中时,能揭示不同变形域的应变特征,从而达到应变分解的目的。  相似文献   

Use of the mantle magnitudeM m for the reassessment of the moment of historical earthquakes     

Emile A. Okal 《Pure and Applied Geophysics》1992,139(1):59-85

The mantle magnitudeM _m is used on a dataset of more than 180 wavetrains from 44 large shallow historical earthquakes to reassess their moments, which in many cases had been previously estimated only on the basis of the earthquake's rupture area. We provide 27 new or revised values ofM _o, based on the spectral amplitudes of surface waves recorded at a number of stations, principally Uppsala and Pasadena. Among them, and most significantly, we document a large low-frequency component to the source of the 1923 Kanto earthquake: the low-frequency seismic moment is 2.9×10²⁸ dyn-cm, in accord with geodetic observations. On the other hand, we revise downwards the seismic moment of the 1906 Ecuador event, which did not exceed 6×10²⁸ dyn-cm.Finally, the study of the 1960 Chilean and 1964 Alaskan earthquakes whose exceptionally large moments are properly retrieved throughM _m measurements, serves proof that this approach performs flawlessly even for the very greatest earthquakes, and is therefore successful in its goal to avoid the saturation effects plaguing any magnitude scale measured at a fixed period.  相似文献   

Internal wave characteristics in the eastern Arabian Sea during summer monsoon     

P G K Murthy  G S Sharma  V V James  K V Suseela 《Journal of Earth System Science》1992,101(4):317-327

The time series BT profiles and surface winds and atmospheric pressure, collected in the deep waters off Ratnagiri and Karwar during summer monsoon were utilized to document the characteristics of internal waves (IW). Low-frequency (≤2, cycle per day (cpd)) IW off Ratnagiri are found to propagate at 83 cm/s with wavelengths of 45 km and wave heights upto 40 m. These parameters for high-frequency (>2 cpd) IW off Karwar correspond to 99 cm/s, 3 km and 23 m. The IW off Karwar appear to leave the station at 70° (±10°) (measured from the horizontal). The data sets were further analysed to address the harmonic composition of the IW and identify the possible sources for the observed IW fields. Power spectra of the IW indicated energy peaks at inertial (0·6 cpd) and tidal (1 and 2 cpd) frequencies off Ratnagiri and in the high-frequency band of 0·5–2·0 cycles per hour off Karwar. The coherence between the IW and wind/tide is found to be good at several frequencies within the IW spectrum. This feature probably suggests tides as a source for the IW of tidal frequencies and winds and tides as a joint source for the IW at the remaining frequencies.  相似文献   

新疆北山地区区域重、磁场特征及其地质意义   总被引：1，自引：0，他引：1  

李四维  张旺生 《新疆地质》1992,(1)

本文在探讨新疆北山地区区域重、磁场特征的基础上,系统地叙述了北山裂谷内发育的白地洼、磁海重力高异常特征和基性、超基性岩体群重、磁场特征。指出坡北、笔架山岩带处于EW、NEE、NNW三组断裂所控制的三角形重力高的梯度带和负磁异常带上。提出通过这一特点,可以在北山地区寻找新的基性、超基性岩体群和拔矿靶区圈定。  相似文献   

Radar observations of prevailing winds and waves in the Southern Hemisphere mesosphere and lower thermosphere     

A. Phillips  R. A. Vincent 《Pure and Applied Geophysics》1989,130(2-3):303-318

HF radar stations (utilizing the spaced-antenna partial-reflection technique) located at Adelaide (35°S, 138°E) and Mawson Station (67°S, 63°E) have observed horizontal mesospheric winds continuously since mid-1984. Observations in the period 1984–87 are compared with the Northern Hemisphere [latitude conjugate] stations of Kyoto (35°N, 136°E) and Poker Flat (65°N, 147°W), and with satellite-derived circulation models. Particular reference is made to the equinoctial changeovers in zonal flow and to the temporal and altitude variations in the planetary wave activity at Mawson and Adelaide.  相似文献