共查询到20条相似文献，搜索用时 78 毫秒
1.
A.M. ZIOLKOWSKI 《Geophysical Prospecting》1980,28(6):902-918
A seismic source array is normally composed of elements spaced at distances less than a wavelength while the overall dimensions of the array are normally of the order of a wavelength. Consequently, unpredictable interaction effects occur between element and the shape of the far field wavelet, which is azimuth-dependent, can only be determined by measurements in the far field. Since such measurements are very often impossible to make, the shape of the wavelet—particularly its phase spectrum—is unknown. A theoretical design method for overcoming this problem is presented using two scaled arrays. The far field source wavelets from the source arrays have the same azimuth dependence at scaled frequencies, and the far field wavelets along any azimuth are related by a simple scaling law. Two independent seismograms are generated by the two scaled arrays for each pair of source-receiver locations, the source wavelets being related by the scaling law. The technique thus permits the far field waveform of an array to be determined in situations where it is impossible to measure it. Furthermore it permits the array design criteria to be changed: instead of sacrificing useful signal energy for the sake of the phase spectrum, the array may be designed to produce a wavelet with desired amplitude characteristics, without much regard for phase. 相似文献
2.
The time-honoured method of attenuating coherent noise in the seismic record is by the use of source and geophone arrays. In theory, and using methods familiar in the synthesis of digital frequency filters, arrays can be designed having virtually any desired response in the wavenumber spectrum. In practice, arrays cannot be implemented with the same precision that is applied in design. The response actually achieved must be compromized by a number of factors. These include inaccuracies in the effectiveness or positioning of individual array elements, variations in ground coupling, and the effect of local heterogenities in the environment of the array. We have no reliable way of knowing how well a particular array will perform from one location to the next. Statistical modelling methods have been applied to examine the effects of implementation errors. Experimental results, supported by statistical theory, show that errors are expected to impose a limit upon the rejection capabilities of an array. The expected limiting value of attenuation due to errors in element weights is inversely proportional to the standard deviation of errors and directly proportional to the square root of the number of array elements. Position errors exert a limiting influence which is wavenumber dependent such that attenuation decreases with increasing wavenumber. For arrays of common dimensions, Gaussian random errors of 10% standard deviation in element weights and positions result in an expected attenuation limit of about 30 dB. It follows that the more ambitious array designs are less tolerant of errors, and must be implemented with greater care and precision in the field. The present work enables us to specify tolerances for any particular array design. Ultimately, the degree of pattern refinement which may be effectively employed in any area is determined by errors which are associated with the array environment. Complex arrays are expensive to operate. In order to avoid over-design it would be useful to establish the magnitude of errors to be expected under different terrain conditions. 相似文献
3.
上海地震台阵的设计方法 总被引：2，自引：2，他引：2
从台阵波数响应特性、子台选址与测试、场地背景噪声分析和记录信号评价等方面，综合对上海地震台阵进行设计，确定了台阵子台的布局点位。本文还介绍了规则台阵与不规则台阵中的几种不同子台布局的台阵波数响应图，并由此得出，采用不规则的子台布局同样可得到性能较好的地震台阵；台阵的子台越多，其响应特性的主峰就越尖锐。 相似文献
4.
J. J. NOOTEBOOM 《Geophysical Prospecting》1978,26(1):194-201
During the last few years many airgun arrays have been designed with the objective of generating a short signature of high amplitude. For linear arrays of non-interacting airguns two rules have been derived that may help in the design or evaluation of airgun arrays. To achieve a short pressure pulse, the total available air volume has to be distributed over the individual guns in such a way that the tail of the signal, owing to the added bubble signals, becomes as flat as possible. When we think of ordering airguns according to volume, this flat signal tail can be achieved by designing the volumes such that the difference in bubble times of two adjacent guns is proportional to their volume to the power 2/3. The amplitude expected from a linear array of non-interacting airguns is limited by the physical length of the array. A graph of measured values tends to confirm this relation. No relation has been found between the total volume of an array and its amplitude. The graph also detects inefficient use of available array length of existing arrays. 相似文献
5.
根据各大网站地震目录和前人研究成果,分析全球地震台网与地震台阵、我国区域台网与地震台阵的监测能力,阐述了地震台阵与密集台网/台阵的区别。研究表明,对同一地区所检测的地震数,地震台阵是地震台网的3-10倍,而震级下限可降低1.2-2级。一般情况下,以微弱信号检测为目的的地震台阵监测能力均优于以结构研究为目的的密集台网/台阵,2种台阵是目的、性质、孔径、形状、台间距、技术手段、研究方法均不同的监测系统。 相似文献
6.
根据汶川地震序列,选出距离合适、波形相关性较好的事件作为震源阵,联合永久台阵(那曲、和田台阵),进行震源阵与固定台阵组合研究,计算其台阵响应.结果表明,地震序列可以形成震源阵,按照地震台阵的特殊方法进行研究,可以提高信噪比,为揭示地下精细结构提供条件. 相似文献
7.
Lei Li 《Journal of Seismology》2011,15(1):165-170
A so-called teleseismic fluctuation wavefield method (TFWM) was adopted by Shen and Ritter to study small-scale heterogeneities
beneath the Lanzhou array, a small-aperture seismic array locating in the northeastern margin of the Tibetan plateau. Through
this method, they speculated a correlation length of 2.4–8.2 km and a root-mean-squared (RMS) velocity perturbation of 1–3%
for the crust under the array. However, for such a tectonically active and heavily deformed region where great earthquakes
up to M7 occurred, such a low RMS velocity perturbation proposed seems to be unconvincing and conflicts with other studies.
To confirm the suspicion, the acoustic finite difference method is used to model scattering wavefields in the random medium
created through parameters suggested by Shen and Ritter. TFWM is applied to the synthetic data from both the small- and large-aperture
arrays. For synthetic data from arrays with similar aperture as the Lanzhou array, it fails to reproduce the parabolic fit
for real data, implying that the statistical parameters proposed by Shen and Ritter are incorrect. Another test presuming
a correlation length of 2.4 km and a RMS velocity perturbation of 5% can reproduce the fit for real data. The numerical experiments
prove that it is improper to apply TFWM to small-aperture arrays like the Lanzhou array, or else the heterogeneity will be
heavily underestimated. The aperture of an array must be much larger than the correlation length and wavelength to get unbiased
measurements. 相似文献
8.
Motivated by several papers by Indian colleagues suggesting that a single-pole array is the most favorable one for locating electrically conductive targets in the underground, detailed measurements were carried out with different electrode arrays over a well-known graphite deposit near Pfaffenreuth, Germany. The following arrays were used: (1) Wenner array; (2) single-pole array; (3) half-Wenner array; (4) half-Schlumberger array. Each of the arrays established the location of the main graphite deposit. The half-Schlumberger array turned out to be the most reliable one since it showed details which were only very poorly indicated by the other arrays or not at all. Mathematical modeling of three-dimensional bodies simulating the geological situation for this deposit were carried out. These results show an unexpectedly good correlation with the measured effects. 相似文献
9.
Songlin Li Xiaoling Lai Zhixiang Yao Qing Yang Geophysical Prospecting Center China Earthquake Administration Zhengzhou China Institute of Geophysics Beijing China 《地震学报(英文版)》2009,(4):417-424
The rupture process of the May 12,2008 MS8.0 Wenchuan earthquake was very complex. To study the rupture zones generated by this earthquake,four dense temporary seismic arrays across the two surface breaking traces of the main-shock were deployed in July and recorded a great amount of aftershocks. This paper focuses on the data interpretation of two arrays across the central main fault,the northern array line 1 and southern array line 3. The fault zone trapped waves recorded by the two arrays were used to st... 相似文献
10.
在哈萨克斯坦的5个现代化数字地震台阵中,4个小孔径同心圆结构的IMS简约型台阵建设、维护方便,全方位监测能力强,1个十字型结构中等孔径台阵,因对特定方位敏感,对更远距离已知核试验点监测能力更强。台阵观测场地均处于完整稳定的构造块体,内部岩石迁移性良好,噪声水平低,保证了对远处微弱地震信号的监测及各子台信号的相似性。地震检波器良好的性能,保证了台阵的地震信号记录质量和数据研究基础。采用卫星传输方式,有效保证了数据的实时性。哈萨克斯坦的地震台阵,其选址、布局、仪器、数据传输等台阵建设,为中国地震台阵发展建设提供了经验借鉴。 相似文献
11.
2D电阻率成像技术近年来被广泛应用于工程、水文、环境和矿产等领域,在实际应用中它具有多种的装置类型,不同的装置类型对特定的地质情况有不同的应用效果.本文通过采用Wenner、Wenner-Schlumberger和dipole-dipole三种排列装置在一个水平和一个垂直模型上正演模拟和块反演,揭示了不同的排列装置在水平结构和垂直结构的异常响应,并对高阻体和低阻体进行了模拟.结果显示当采用Wenner,Wenner-Schlumberger和dipole-dipole数据采集技术时,不同的模型结构异常响应有明显的不同,三种排列类型对地下低阻体的分辨能力均高于高阻体,Wenner装置和dipole-dipole装置分别对水平层状结构和垂直结构有较好的分辨力,wenner-Schlumberger装置对水平层状结构有好的分辨力,对垂直结构有中等的分辨能力. 相似文献
12.
多年来,胜利探区多波多分量地震采集所得资料的信噪比和分辨率较低,无法取得较好的应用效果.为此,以胜利垦71区块为先导实验区开展了多波采集方法研究.首先,通过单点三分量检波器与常规检波器小面积组合分析了该区转换波发育情况,认为该区转换界面较强,转换波特征明显,转换横波速度约为纵波速度的1/2;然后,通过数字三分量检波器的室内各种组合研究,进行了超线元叠加,由此可以有效地改善资料的信噪比,并对分辨率基本没有影响;最后,利用三分量检波器扩展排列进行转换波最佳偏移距的设计,通过垂直排列追踪放炮进行最佳非纵距设计,从而得出该区多波采集的最佳观测系统参数.通过上述合理的设计和多项试验研究,在垦71地区多波采集中,数字检波器Z分量剖面的频率优势非常明显,分辨率明显高于常规检波器的纵波剖面,对于搞清小断层及微幅度构造具有重要的意义;同时,转换横波能量强、信噪比和分辨率高,使多波采集取得了较好的效果. 相似文献
13.
利用高密度电阻率法确定滑坡面的正演研究 总被引：2，自引：0，他引：2
高密度电法探测是滑坡面探测的有效手段,适宜 的现场工作方案和相应的资料解译模型,是获取 可靠探测成果的前提。本文针对高密度电法勘探 中常用的四类电极排列方式,即维纳、施伦贝谢、 偶极、二极,利用有限元的方法二维正演模拟建 立了均质土坡滑面、软弱夹层滑面、堆积层滑面、 构造破碎带滑面的标准地电模型剖面;明确了进 行不同类型滑坡工程地质调查时不同电测装置的 探测能力和视电阻率异常模式;提出复杂地质条 件下斜坡问题探测数据有效处理的设计比值参数 方法。最后给出若干利用高密度电阻率法进行滑 坡工程地质调查的典型实例。 相似文献
14.
TXAR台阵位于美国德克萨斯州,是IMS下属的主要地震台阵之一。该台阵将台站数目压缩到9个,采用无线遥测通讯方式,减少了建设和运行维护成本。其地震计室采用钻孔加套管的形式,具有安装简易、密封性好的优点。台阵采用无人值守设计,使用太阳能板、UPS电池和燃油发电机等多种供电方式,具有可靠稳定的性能。 相似文献
15.
Sándor Szalai László Szarka 《Journal of Applied Geophysics》2011,75(1):1-8
Recent two-dimensional multielectrode measurements are restricted to only a few geoelectric arrays. Realizing that specific features of nearly 90 other arrays are totally ignored, all original intentions as published about the development of new geoelectric arrays were reviewed. Apart from arrays, either already applied in two-dimensional geoelectric arrays or impossible to be applied in such systems, 61 forgotten once-developed arrays were found. These provide altogether 102 various solutions, which would be able to increase the efficiency of two-dimensional multielectrode measurements in some respect. 46 array solutions are able to enhance the depth of investigation; 9/11 array solutions give better vertical/horizontal resolution; 17 array solutions provide better planview images; 8 array solutions are worth applying in areas with limited access; 11 array solutions may reduce the effect of near-surface inhomogeneities. By reviving these forgotten arrays, it will be possible to develop versatile multielectrode systems, which are more adaptive to the diverse field needs. 相似文献
16.
In recent years, the use of wide source arrays in marine seismic surveys has been a topic of interest in the seismic industry. Although one motivation for wide arrays is to get more guns in a source array without increasing the in-line array dimension, wide arrays can also provide the benefit of suppressing side-scattered energy. Comparisons of common midpoint (CMP) stacks of data acquired offshore Washington and Alaska with wide and conventional-width source arrays, however, show only small and sometimes inconsistent differences. These data were acquired in areas where side-scattered energy is a problem. Comparisons of pre-stack data, however, show substantial differences between the wide and conventional source array data. The disparity between the stacked and prestack data is explained by analysing the effective suppression of back-scattered energy by CMP stacking. Energy reflected from scatterer positions broadside to a given CMP location has a lower stacking velocity than that of the primary reflection events. Thus, CMP stacking attenuates the side-scattered energy. In both survey areas the action of CMP stacking was so powerful in suppressing the broadside energy that the additional action of the wide array was inconsequential in the final stacked sections. In other areas, where the scattering velocity is comparable to the primary stacking velocity, wide arrays could provide considerable advantage. Even though CMP stacked data from wide and conventional-width arrays may appear similar, the reduced amount of side-scattered energy in wide-array prestack data may provide a benefit for data dependent processes such as predictive deconvolution and velocity analysis. However, wide arrays cannot be used indiscriminately because they can degrade cross-dipping primary events. They should be considered primarily as a special tool for attacking severe source-generated noise from back-scattered waves in areas where the action of CMP stacking is insufficient. 相似文献
17.
概述了国内外强震动观测的研究现状和结构地震反应观测台阵的研究情况。并对北京市人大办公楼的结构地震反应观测台阵的研究实例作了分析,该观测台阵在没有强震的情况下,依然取得了有用的地震记录。文中对该台阵得到的两次地震记录分析、处理,结果的对比分析用于验证该结构反应观测台阵布设的合理性。最后阐述了该台阵布设的不足,针对不足给出几点结构反应观测台阵布设的合理建议,并展望了结构地震反应观测台阵布设研究的美好前景。 相似文献
18.
We present results from laboratory experiments on flow through submerged arrays of rigid cylinders embedded in a sandy bed. Using rigid, cylindrical elements to mimic vegetation and benthos, we account for only the physical effects resulting from their presence, eliminating biological factors, such as biofilms and root systems. In line with previous findings, rigid arrays modify the flow mean and turbulent velocity statistics. However, even if the flow speed is significantly damped within dense arrays, the amount of sediment that gets lifted into suspension increases as the density of the array increases due to array– and cylinder-scale turbulence. We present a first attempt to provide predictive relationships of suspended sediment concentration using an alternative approach for the Shields parameter with an empirical coefficient to account for turbulence generated by submerged arrays of rigid cylinders. A similar analysis, using a ratio of populated to non-populated Shields parameter, is conducted to predict resuspension as a function of array density. 相似文献
19.
Seismic array can be traced back to 1950s when it mainly aimed at detecting and distinguishing the signals of nuclear explosion and seismic signals. The research on seismic array includes seismic array techniques and applications of array in geophysics. Array techniques involve array design and data processing methods (Anne, 1990). Nowadays, the continuous development of seismic array￠s theory could relate to many scientific issues in geophysical field (Tormod, 1989; Mykkeltveit, Bungum, 1984).
Seismic array is mainly applied to detect weak events. The response characteristic of array is an important indication of array￠s detection ability. Therefore, when we study an array or construct an array, one of the neces-sary works is to calculate the response characteristics of the array (Harjes, 1990).
The aperture and layout of array are two dominating geometrical features. The typical aperture of interna-tional array is generally from several to tens kilometers. For instance, arrays with aperture of dozens kilometers aperture are KSA, WRA, YKA, etc, while arrays with several kilometer aperture are ARC, FIN, GEE, etc. Moreo-ver, in the view of array￠s layout, NOR, GER, etc have circle layout, while WRA, YKA, etc have decussating layout.
This paper mainly discusses the relation between deployment of array and wavenumber response. With the example of constructing Shanghai Seismic Array, this paper provides one practical solution to search the proper array deployment. In this paper, the simple delay beam technique is adopted to calculate the response characteris-tics of array. Certainly, the different processing methods have different result, but the result from the simple delay beam processing could be enough to reflect the feature of an array. 相似文献
20.
JAN HELGESEN 《Geophysical Prospecting》1991,39(3):313-336
Three methods for least-squares inversion of receiver array-filtered seismic data are investigated: (1) point receiver inversion where array effects are neglected; (2) preprocessing of the data with an inverse array filter, followed by point receiver inversion; (3) array inversion, where the array effects are included in the forward modelling. The methods are tested on synthetic data generated using the acoustic wave equation and a horizontally stratified earth model. It is assumed that the group length and the group interval are identical. For arrays that are shorter than the minimum wavelength of the emitted wavefield, and when the data are appropriately muted, point receiver inversion (first method) gives satisfactory results. For longer arrays, array inversion (third method) should be used. The failure of the inverse array filter (second method) is due to aliasing problems in the data. 相似文献