共查询到20条相似文献，搜索用时 437 毫秒
1.
R.D. OGILVY 《Geophysical Prospecting》1987,35(4):454-473
Theoretically exact type curves for a semi-infinite thin conductor are presented for various dip, angles, depth of burial and conductance. The study shows that the common-loop response shape is sensitive to small changes in conductor dip, but is affected more subtly by comparable strike variations. For large sheet conductors a decrease in the strike angle results in a broadening but unlike that for a finite plate there is no reduction in peak amplitude. For dipping conductors, response asymmetry and the direction and magnitude of peak amplitude displacement can be used to assess the disposition and quality of the conductor. A generalized interpretation scheme is proposed, based on dimensionless response characteristics and normalized decay curves, to facilitate the rapid in-field determination of conductor dip, conductance and depth of burial, for any time regime. 相似文献
2.
The interpretation of VLF-EM surveys in terms of buried conductors can be assisted by the application of a linear filter to the observed in-phase component of the vertical magnetic field. One such scheme is examined critically by using the calculated response from a variety of synthetic models to compute theoretical current density pseudosections. The results confirm that this filter technique provides a useful complementary tool for studying the third (i.e. depth) dimension. For single, steeply dipping plates (> 45°) diagnostic information may be derived concerning the depth, size, lateral location, and direction of dip, since the current density maxima seems always to occur within the conductor or at least within one data interval. However, there are some limitations which do not appear to be widely recognized. For single plates the angle of dip cannot be resolved by the current density transformation. Pattern distortions can occur where targets are in close proximity, where the cross-sectional form of the conductor is complex or where the dip is shallow (< 45°). In these latter cases the current density maxima may not occur within the conductive structure and therefore cannot be used to infer depth of burial and/or conductor shape with the same degree of confidence. 相似文献
3.
The response of a rectangular plate to the Crone PEM system has been investigated for different values of depth, dip and conductance parameters. The conductance aperture diagram is presented to estimate the conductance and depth to the top of a vertical sheet. Information regarding dip and depth may be obtained using the appropriate nomogram. 相似文献
4.
Induced polarization and resistivity model studies over thin dykes for varying resistivity contrasts, depth of burial, and dip angles show striking parallelism of the surface apparent resistivity contours with the boundary of the body. This effect may be utilized for the estimation of strike length of the body. Results show that intermediate values of the electrode spacing is satisfactory for detection under widely varying conditions of resistivity contrast and depth. The percentage frequency effect (P.F.E.) and the metal factor (M.F.) responses are found to be more sensitive to the variation in the depth of burial than the resistivity responses. Pseudosections for P.F.E. and M.F. are concentrated much closer to the body than the resistivity pseudo-sections. 相似文献
5.
Somala Surendra Nadh Chanda Sarit Raghucharan M. C. Rogozhin Evgenii 《Journal of Seismology》2021,25(5):1339-1346
Journal of Seismology - A multi-layer perceptron (MLP) technique is used to train on the response spectra for various strike angles, dip angles, and rake angles. Fixing the magnitude and depth of... 相似文献
6.
In a weathered environment estimates of depth and conductance of metallic sulphide dykes from conventional anomaly index diagrams for a vertical half-plane in air have to be corrected, besides the usual corrections, for: 1. moderate conductivity of the host rocks, and 2. finiteness of strike length S and depth extent D. Model experiments have been carried out to evaluate the response variation of a vertical planar conductor with varying depth extent and strike length for both insulating and conductive surroundings. The results indicate: 1. A conductor with finite depth extent (D/L < 2.5) or strike length (S/L < 5.0) in an insulating medium yields a lower estimate of conductance (mineralization) and a greater depth. 2. A moderately-conductive host rock enhances the anomaly and rotates the phase so that the conductor appears to be more resistive (less mineralized) and shallower. The results have practical significance since in weathered surroundings a highly-mineralized body of finite size could be missed, or misjudged, because of low estimates of conductivity and depth. 相似文献
7.
2021年7月18日—8月7日,宁夏吴忠—灵武地区发生ML3.6显著震群活动。本文利用多阶段定位方法对该震群进行了重新定位,并根据gCAP方法反演了2021年7月20日灵武ML3.6地震的震源机制及震源矩心深度,采用Snoke方法计算了震群中3次ML3.0以上地震的震源机制,测定了同一地震多个震源机制的中心解。结果表明,该震群中最大的地震即7月20日02时40分ML3.6地震的震源机制为节面Ⅰ走向289°,倾角72°,滑动角?22°,节面Ⅱ走向26°,倾角69°,滑动角?161°,震源矩心深度为12 km,初始破裂深度为12.5 km;7月20日03时15分ML3.2地震的震源机制为节面Ⅰ走向290°,倾角82°,滑动角?2°,节面Ⅱ走向20°,倾角88°,滑动角?172°,初始破裂深度为11.9 km;7月21日04时55分ML3.1地震的震源机制为节面Ⅰ走向285°,倾角53°,滑动角2°,节面Ⅱ走向194°,倾角88°,滑动角143°,初始破裂深度为11.6 km,这些地震震源机制的主压应力轴主要为NE向。该震群序列的震源深度主要相对集中在7—15 km之间,其中ML3.0以上地震的震源深度主要介于11—13 km,震源深度剖面显示震群相对集中的区域由深到浅大体呈现近似于陡立的展布。本文进一步研究发现区域应力场在灵武ML3.6地震震源机制NNE向节面产生的相对剪应力为0.393,而在NWW向节面产生的相对剪应力为0.945。结合地质构造和已有断层资料初步分析认为,若NNE向的崇兴隐伏断裂为灵武ML3.6地震的发震断层,则表明崇兴断裂可能是一条断裂薄弱带,地震破裂方式主要为右旋走滑;若NWW向的未知隐伏断裂为发震断层,则表明NWW向断裂可能为该地震在区域应力场下的剪应力相对最大释放节面,其破裂方式为左旋走滑。 相似文献
8.
M. PODDAR 《Geophysical Prospecting》1982,30(1):86-100
A survey using Crone pulse electromagnetic (PEM) equipment was conducted near the village of Gani in Andhra Pradesh, India. The anomalies obtained had a shape typical for an inclined sheet conductor. From the multichannel TEM response, the multifrequency Slingram response was calculated. A comparison of the Slingram response of the Gani conductors with the free-air model response of a thin sheet conductor shows phase rotation and attenuation of the anomaly vector, thereby confirming the presence of a conductive overburden. Interpretation of the Gani results using free-air phasor diagrams causes an overestimation of depth and conductance of the target conductor unless data obtained at a sufficiently low frequency are used for the interpretation. For areas like Gani this frequency can be as high as 336 Hz. 相似文献
9.
P. HUBRAL 《Geophysical Prospecting》1976,24(3):478-491
Various Dix-type formulae are derived, which are useful to approximate travel time functions that can be observed while modeling the common depth point (CDP) technique for 3-D isovelocity layers of varying dip and strike. All formulae can be used to compute interval velocities and recover the depth model from surface measurements. They are established by making use of the concept of wavefront curvature. Many similarities with known formulae valid for the 2-D plane isovelocity layer case exist. 相似文献
10.
对印尼地区3574次M≥5.0地震震源断层面上的海潮负荷应力进行计算,研究了地震断层上的负荷应力随深度变化以及随断层倾角和走向的变化特征.结果表明,地震断层上的负荷正应力大于负荷切应力.逆断层上的负荷应力最大,其它依次为斜滑断层、正断层和走滑断层.倾角范围在0°—50°的断层上的负荷正应力随倾角增大有减小趋势,负荷切应力在30°—50°倾角范围的断层上较大.负荷应力随断层走向的趋势性变化不明显.不同类型断层上的负荷正应力和切应力在震源深度15km处均达到最大,之后随深度增加而减小.当震源深度小于40km时,断层面上的海潮负荷应力的量级与固体潮应力相当.因此指出,在潮汐应力对地震影响的研究中,对震源深度小于40km的海洋和沿海地震,除固体潮汐应力外还需要考虑海潮负荷应力的影响. 相似文献
11.
Yongge Wan Zheng-kang Shen Min Wang Yuehua Zeng Jichao Huang Xiang Li Huawei Cui Xiwei Gao 《地震科学（英文版）》2015,28(3):187-195
We analyze co-seismic displacement field of the 26 December 2004, giant Sumatra–Andaman earthquake derived from Global Position System observations,geological vertical measurement of coral head, and pivot line observed through remote sensing. Using the co-seismic displacement field and AK135 spherical layered Earth model, we invert co-seismic slip distribution along the seismic fault. We also search the best fault geometry model to fit the observed data. Assuming that the dip angle linearly increases in downward direction, the postfit residual variation of the inversed geometry model with dip angles linearly changing along fault strike are plotted. The geometry model with local minimum misfits is the one with dip angle linearly increasing along strike from 4.3oin top southernmost patch to 4.5oin top northernmost path and dip angle linearly increased. By using the fault shape and geodetic co-seismic data, we estimate the slip distribution on the curved fault. Our result shows that the earthquake ruptured *200-km width down to a depth of about 60 km.0.5–12.5 m of thrust slip is resolved with the largest slip centered around the central section of the rupture zone78N–108N in latitude. The estimated seismic moment is8.2 9 1022 N m, which is larger than estimation from the centroid moment magnitude(4.0 9 1022 N m), and smaller than estimation from normal-mode oscillation data modeling(1.0 9 1023 N m). 相似文献
12.
In the quantitative data interpretation for HLEM induction prospecting, a vertical half-plane model in an insulating medium is widely employed. For this assumption to be valid, the steeply dipping massive sulphide dykes must have large strike lengths and depth extents, but small thickness. We report investigations, using the laboratory scale-modelling method, on the response variation of large vertical conductors as the thickness is varied. We conclude that a steeply dipping large dyke can be approximated by a half-plane model only if its thickness is less than half the skin depth. An inductively thick conductor produces larger amplitudes and relatively higher quadrature compared to a thin conductor, even if both have the same induction number. 相似文献
13.
The magnetometric resistivity (MMR) method uses a sensitive magnetometer to measure the low-level, low-frequency magnetic fields associated with the galvanic current flow between a pair of electrodes. While the MMR anomalies of simple structures such as dikes and vertical contacts have been determined analytically, there is a lack of systematic information on the expected responses from simple three-dimensional bodies. We determine the characteristic anomalies associated with square, plate-like conductors, which are excellent models of many base metal mineral deposits. The anomalies of plates of finite size are determined numerically using an integral equation method. A plate is subdivided into many sections and the current flow within each section is solved by equating the electrical field within each section to the tangential electrical field just outside it. When the plate size is small in relation to either the depth or the transmitter spacing, the shape and amplitude of the anomaly produced is closely approximated by a current dipole model of the same length and depth. At the other extreme, a large plate is represented by a half-plane. The dipole and half-plane models are used to bracket the behaviour of plates of finite size. The form of a plate anomaly is principally dependent on the shape, depth and orientation of the plate. A large, dipping plate near the surface produces a skewed anomaly highly indicative of its dip, but the amount of skew rapidly diminishes with increased depth or decreased size. Changes in plate conductivity affect the amplitude of the anomaly, but have little effect on anomaly shape. A current channelling parameter, determined from the conductivity contrast, can thus be used to scale the amplitude of an anomaly whose basic shape has been determined from geometrical considerations. The separation into geometrical and electrical factors greatly simplifies both the interpretation and modelling of MMR anomalies, particularly in situations with multiple plates. An empirical formula, using this separation, predicts the anomaly of two or more parallel plates with different conductances. In addition, the relation between the resolution of two vertical, parallel plates of equal conductance and their separation is determined. The ability of the integral equation method to model plate-like structures is demonstrated with the interpretation of an MMR anomaly in a survey conducted at Cork Tree Well in Western Australia. The buried conductor, a mineralized graphitic zone, is modelled with a vertical, bent plate. The depth to the top of the plate, and the plate conductance, is adjusted to fit the anomaly amplitude as closely as possible. From the modelling it would appear that this zone is not solely responsible for the observed anomaly. 相似文献
14.
PETER FURNESS 《Geophysical Prospecting》1993,41(1):113-130
Furness , P. 1993. Gradient Array Profiles over thin resistive veins. Geophysical Prospecting 41 , 113–130. Gradient array geoelectric surveys are commonly used to explore for buried sheet-like targets. It is demonstrated that under certain circumstances the responses of such features can become practically equivalent for a range of models differing considerably in resistivity and thickness. This is the dual of the familiar equivalence phenomenon associated with thin beds in geoelectric sounding operations. Hence the geoelectric response profiles over thin dipping resistive veins are conveniently studied by considering equivalent forms with vanishing thickness and infinite resistivity but with the same resistivity-thickness product. The effects of varying the dip, depth of burial, depth extent and resistivity–thickness product of such features on the gradient array response profiles are investigated by means of a series of numerical experiments. These demonstrate several effects of significance to survey design and data interpretation. In particular it is found that while the resistivity–thickness product influences the amplitude of the response profiles it has little effect on their form. A similar behaviour is found to be exhibited by veins with extended depth extent when the dip is varied. A complete quantitative interpretation of gradient array profiles over thin dipping resistive veins is thus only possible for veins of limited depth extent. For veins with an extended depth dimension, the data is ambiguous (in a practical sense) in terms of the dip and the resistivity–thickness product. Here, the interpretation can only be expected to deduce the horizontal and vertical locations of the vein apex. 相似文献
15.
2020年6月9日宁夏中卫市沙坡头区发生ML3.4地震,该地震发生在1709年中卫南7?级地震的极震区内,且震中位于以往弱震相对偏少的地区。本文利用宁夏区域地震台网的波形记录,采用gCAP方法反演了2020年6月9日中卫ML3.4地震的震源机制解及震源矩心深度,并用Hash方法计算其震源机制解,且得出了两种方法的震源机制中心解。结果表明,gCAP方法的震源机制解为:节面I走向255°,倾角79°,滑动角?20°;节面II走向348°,倾角70°,滑动角?168°,震源矩心深度为12 km。而Hash方法的震源机制解为:节面I走向344°,倾角89°,滑动角176°;节面II走向74°,倾角86°,滑动角1°。两种方法的震源机制中心解为:节面I走向255°,倾角87°,滑动角?11°;节面II走向346°,倾角80°,滑动角?176°,主压应力轴走向主要为NE向,其中gCAP方法结果与震源机制中心解的最小空间旋转角相对最小,为12.09°。结合过去地质构造资料,推测2020年6月9日中卫ML3.4地震的主要错动方式为左旋走滑,且断层面为NEE向节面的可能性较大。 相似文献
16.
吴宝峰 《地震地磁观测与研究》2017,38(6):26-29
利用西藏地震台网记录的波形数据,采用CAP方法,反演2017年11月18日西藏米林M 6.9地震震源机制解,并绘制余震空间分布。反演得到,节面Ⅰ：走向285°,倾角47°,滑动角70°;节面Ⅱ：走向133°,倾角46.6°,滑动角110.1°,矩心深度约19.0 km。结果显示,此次地震是逆冲为主兼少量走滑型地震,节面Ⅰ走向与NW向嘉黎—察隅断裂走向一致,余震空间展布也与断裂走向一致。 相似文献
17.
V. I. Vlodavetz 《Bulletin of Volcanology》1971,35(2):470-478
The Turja Peninsula consists of porphyritic granite overlain by sandstone, cut by numerous dikes and veins of varying composition, form, and orientation. The relative ages of the dikes and veins has been established by their mutual intersections, and correlation of these with compositions of the rocks demonstrates the existence of three periods of igneous activity. The dikes and veins of the first period strike predominantly NNE and dip ESE. Most of those of the second period strike E-W and dip N, but those of a subordinate group strike NNE and dip ESE. Those of the third period strike predominantly N-S and dip E. The first and third periods are characterized by fine grained rocks resembling effusives, the second by coarse grained typically intrusive rocks and intense metasomatism that altered both dikes and veins and the wall rocks. The difference in texture of rocks formed at the same depth horizon is attributed to a difference in temperature of the wall rocks and the rate of rise of the magma through them. 相似文献
18.
Finding the strike direction of fractures using GPR 总被引：3，自引：0，他引：3
Soon Jee Seol Jung-Ho Kim † Yoonho Song‡ Seung-Hwan Chung§ 《Geophysical Prospecting》2001,49(3):300-308
GPR reflection energy varies with antenna orientation relative to the strike and dip of the reflector. This directional dependence of GPR responses was investigated through numerical experiments and was used to estimate the azimuth of fractures and joints. Three antenna configurations were considered in this study: perpendicular-broadside (YY mode), parallel-broadside (XX mode) and cross-polarization (YX mode). The reflection energy in the cross-polarization mode shows a shape characteristic similar to the strike, regardless of the dip angle. Those in the other two modes show quite different amplitudes from the strike, depending on the dip angle. We have developed a strike-direction-finding scheme using data obtained from the three different modes for the same survey line. The azimuth angle of each reflector was displayed in colour on the GPR profile. This scheme was applied to a field survey at a granite quarry in southern Korea. The GPR profiles showed different images of the reflectors depending on the antenna configuration. The estimated azimuths of reflectors obtained using our scheme matched fairly well with those of known fractures and joints. 相似文献
19.
本文以海原断裂带区域活动构造为基础,将海原断裂划分为西、中、东3段.基于1999年12月26日至2010年7月26日间的精定位小震目录,估计了海原断裂带各段的倾角.考虑海原断裂沿走向可能存在南倾与北倾两种情况,将倾角的范围设置为.首先运用网格搜索法确定了平面断层模型,其次以特征深度节点为基础数据运用多项式构建了曲面断层模型.结果表明：当进行平面拟合时,海原断裂西段与中段、东段的倾向不同,西段为南倾,其倾角值为71°,而中段、东段为北倾,其倾角值分别为72°、65°,各段的倾角值均由地表以下8 km地震资料确定.当进行曲面拟合时,在8 km深度以内海原断裂西段、中段、东段的倾角均处于80°左右,即接近陡立.西段的倾角在深度为9 km处出现转换,之后倾角接近陡立;中段的倾角在深度为16 km处出现转换,之后倾角逐渐减小,当深度为18 km时倾角为30°;东段的倾角在深度为11 km处出现转换,倾角为42°,在深度为16 km处出现第二次转换,倾角为55°,之后倾角逐渐减小.结合震源机制解和大地测量观测资料反演拟合的合理性,验证了本文所估计倾角的可靠性. 相似文献
20.
One of the significant problems of modern deep magnetotellurics is the recognition of anisotropy in the crustal and mantle
conductive zones. In the paper we perform numerical experiment comparing several 2D models of crustal and mantle isotropic
and anisotropic prismatic conductors. Anisotropy is modeled by alternating horizontal or vertical thin layers of different
resistivities (the vertical layers are parallel to the prism strike). Using these models, we examine conditions under which
the magnetotelluric and magnetovariational response functions distinguish between isotropy and anisotropy. The resolution
of MT and MV studies depends on the sediments conductance, lithosphere resistance and deep conductor width. Calculations show
that the most favorable conditions for anisotropy studies are observed in the active regions characterized by small sediments
conductance (10–20 S) and moderate lithosphere resistance (108 Ohm·m2). However, in the stable regions, where sediments conductance exceeds 50–100 S and the lithosphere resistance comes up to
109 Ohm·m2, the crustal and mantle anisotropic and isotropic conductors manifest themselves in the equivalent magnetotelluric and magnetovariational
functions, which cannot distinguish between anisotropy and isotropy and admit both the interpretations. 相似文献