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1.
潮间带周期性淹水区域水深、流速的变化过程是潮滩水动力过程的基本组成部分,也是潮流与泥沙相互作用的基础。通过2002年4月至2003年1月4个季节的野外实测,获得了平静天气条件下,崇明东滩滩面潮流水深、流速与流向的变化过程数据。结果表明,崇明东滩盐沼和邻近光滩处涨潮历时均小于落潮历时,水深过程变化呈现出“陡涨缓落”的特点。光滩与盐沼交界处光滩一侧流速过程呈“双峰型”特征,涨落潮均出现流速峰值;盐沼（植物生长期）流速过程具有“单峰型”特点,仅在涨潮初出现峰值。研究区潮流不对称性明显,主要表现为涨潮优势,且由光滩向盐沼上部不断增强,潮沼植物和地形变化是加强盐沼区涨潮优势的主要原因。流速变化过程的差异和潮流不对称性使盐沼区域发生稳定的泥沙淤积,盐沼前缘光滩则会出现较频繁的冲淤变化,平静天气条件下,它们是控制崇明东滩泥沙输移和潮滩动力地貌过程的动力基础。 相似文献
2.
The key features in the distribution of geoelectric and velocity heterogeneities in the Earth’s crust and the upper mantle of Kamchatka are considered according to the data of deep magnetotelluric sounding and seismotomography. Their possible origin is discussed based on the combined analysis of electric conductivity and seismic velocity anomalies. The geoelectric model contains a crustal conducting layer at a depth of 15–35 km extending along the middle part of Kamchatka. In the Central Kamchatka volcanic belt, the layer is close to the ground surface to a depth of 15–20 km, where its conductivity considerably increases. Horizontal conducting zones with a width of up to 50 km extending into the Pacific Ocean are revealed in the lithosphere of eastern Kamchatka. The large centers of current volcanism are confined to the projections of the horizontal zones. The upper mantle contains an asthenospheric conducting layer that rises from a depth of 150 km in western Kamchatka to a depth of 70–80 km beneath the zone of current volcanism. According to the seismotographic data, the low- and high-seismic-velocity anomalies of P-waves that reflect lateral stratification, which includes the crust, the rigid part of the upper mantle, the asthenospheric layer in a depth range of ~70–130 km, and a high-velocity layer confined to a seismofocal zone, are identified on the vertical and horizontal cross sections of eastern Kamchatka. The cross sections show low-velocity anomalies, which, in the majority of cases, correspond to the high-conductivity anomalies caused by the increased porosity of rocks saturated with liquid fluids. However, there are also differences that are related to the electric conductivity of rocks depending on pore channels filled with liquid fluids making throughways for electric current. The seismic velocity depends, to a great extent, on the total porosity of the rocks, which also includes isolated and dead-end channels that can be filled with liquid fluids that do not contribute to the electric-current transfer. The data on electric conductivity and seismic velocity are used to estimate the porosity of the rocks in the anomalous zones of the Earth’s crust and the upper mantle that are characterized by high electric conductivity and low seismic velocity. This estimate serves as the basis for identifying the zones of partial melting in the lithosphere and the asthenosphere feeding the active volcanoes. 相似文献
3.
叠加速度成图在CPS3绘图系统中的实现 总被引：1，自引：0，他引：1
基于CPS3绘图系统的工作原理和常规时深转换,针对目的层埋藏深,速度横向变化大,钻孔资料少的三维勘探区,摸索出了一套由叠加速度出发进行时深转换的方法。此方法成功地应用于华北煤田TSK勘探区的三维资料解释中,弥补了传统时深转换方法的不足,收到了很好的效果,所绘制的构造图深度同巷道资料吻合。 相似文献
4.
渤中凹陷BZ1探区Qa构造两口钻井在相距1.3 km的实钻过程中出现了速度异常,三维地震资料时间剖面地层深度与钻井地质分层深度出现了不一致的矛盾现象,即新钻井Qa 3井的钻井预测深度相对于本井地质分层深度更深,速度相对于Qa 2井变小,因而两口井地震速度在横向分布上出现了明显差异。分析表明,速度异常主要由沉积和构造共同作用所引起。利用地震叠加速度谱建模,通过井点速度场、趋势种子点进行校正,获取到更加准确的地下速度,并进行高精度变速成图,能够真实反映地下构造。对比单井速度预测钻井深度与单井速度场校正速度谱建模速度场预测钻井深度,并对比其误差精度,可以看出后者有效地解决了实际钻探过程中因速度异常而导致预测深度误差偏大的问题。因此钻前进行速度场建模与变速构造成图,对今后勘探井或评价井的部署及钻井深度精确预测具有重要的指导作用。 相似文献
5.
The water column flow velocity of 36 river sections in the river reach between Hankou (Wuhan) and Wuxue of the middle-lower
Changjiang River. Their cross sectional distribution patterns in relation to the river channel morphologies were examined
by using ship-mounted ADCP (Acoustic Doppler Current Profiler) instrument. The results indicate four (I-VI) types of river
channel morphology associated flow patterns: I—laterally deepening riverbed topographic pattern; II—symmetrical to asymmetrical
riverbed topographic pattern; III—relative flat riverbed topographic pattern, and IV—sandbar supported riverbed topographic
pattern. All these correspond to the different patterns of flow velocity distribution. The maximum flow velocity is usually
related to the deeper water depth, but irregular water column distribution of flow current velocity results often from the
vortices’ current associated with river knots. Deeper river water depth is usually identified in the river reach located slightly
downstream to the river knot, where faster flow velocity occurs. Downward change in flow velocity fits semi-log law, showing
an exponential decreasing flow current with the maximum flow velocity near the water surface. However, in the river reach
near the river knots, the water column distribution of flow current velocity does not fit the semi-log law, showing the irregular
flow current pattern. This study, in context of river catchment management, highlights the controls of riverbed morphology
to the flow current structure, which will shed light on the post study of Three Gorges damming in 2009. 相似文献
6.
D. MARC AUDET 《Sedimentology》1995,42(2):355-373
A continuum mechanics model for the gravitational compaction of sediments is derived by assuming that the sediments are normally pressured and in a one-dimensional state of stress. Sediment strength is characterized in terms of effective stress laws adopted from soil mechanics. The model is a relatively simple mathematical formula that gives the porosity as a function of burial depth. The shape of the porosity profile is controlled by two mechanical parameters, the compression index and the void ratio at an effective stress of 100 kPa. The model was verified by analysing the porosity—depth data of oozes and chalk from the Ontong Java Plateau, gathered during Leg 130 of the Ocean Drilling Program. The mechanical parameters of the sediments were estimated using a least-squares method to fit the theoretical profile to the porosity data. The theoretical profile described accurately the ooze porosity data over depth ranges of 100 m or more. However, over smaller length-scales of 10–50 m there were systematic deviations between the theoretical porosity values and the ooze porosity data. The porosity deviations correlated with variations in the mean grain size of the sediments, due in part to changes in the foraminifera abundance. In the case of the oozes, the estimated mechanical parameters were consistent with published values obtained from one-dimensional compression tests. In contrast, the estimated mechanical properties for the chalks differed from published values. The chalk porosities were lower than could be explained by mechanical compaction. This explanation is supported by the compressional (P-wave) velocity data. In the chalk sections, the P-wave velocity increases more rapidly with burial depth than it does in the ooze sections, suggesting that sediment elastic properties are increasing due to interparticle binding. 相似文献
7.
稳态瑞利波勘探所能达到的勘探深度是众多使用者越来越关心的话题。作者依据瑞利波勘探的基本原理和多年的实践经验,对影响勘探深度的各种因素,包括岩层的平均速度vR、使用的最低频率fmin、震源能量、各种地质因素、耦合因素等一一作了分析,并列举了多种条件下勘探深度的实际数据。指出综合运用合理参数,进一步提高对小异常的识别能力,有可能在目前基础上把瑞利波方法的勘探深度再提高一步。 相似文献
8.
确定起伏地表的空间位置是叠前深度域起伏地表偏移成像和速度建模成功的关键.浮动基准面本身就是一个起伏高程面,此外它还定义了CMP道集在其上进行基准面校正的规则.本文分析了确定浮动基准面的常用方法并明确了其在一般情况下所具有的物理意义,指出了即便是基于平均静校正法得到的浮动基准面,在一定条件下也可以直接用于起伏地表叠前深度... 相似文献
9.
l.IntroductionAteleseismicprofilingwasconductedjointlybytheChineseAcademyofGeologicalSciencesandtheInstitUteofGeophysicsandInnerTectonics,JosephUniversity,France,alongthemainroadfromGonghetoYushuinQinghai,withanarrayof4Othree-componentMinititanstationsandl3one-componentCEISstations,fromJunetoNovember,1998.ThestUdycoversahugearearangingfromthenofthoftheBangong-NujiangFaulttothesouthoftheMid-QilianFault,andfromtheeastoftheQaidamBasintothewestoftheLongmenShanFault,goingthroughSouthQ… 相似文献
10.
During 1976 the first installment of a long range seismic profile was conducted in the North Pacific to a range of 600 km using shots to two tons in size. The line was shot to a closely-spaced array of Scripps ocean bottom seismographs and was parallel to magnetic anomaly 32 at an age of approximately 70 · 106 yr. The line extended between the Clarion and Molokai Fracture Zones and did not cross any major topographic features. Linearized and extremal travel-time inversions were conducted to provide bounds on the compressional velocity as a function of depth. The velocity does not exceed 8.4 km s−1 to a depth of 60 km at which point the data no longer provide any resolution. The constraints on the acceptable models were improved by using array processing methods to measure phase velocity and synthetic seismogram techniques to model phase and amplitude information. The oceanic crust is composed of a series of gradients with no first order discontinuities. The “Moho” is smeared out over a depth of 1.5–2.0 km even though “wide-angle reflections” from the Moho, the phase PMP, are clearly seen in the data. The upper lithosphere is characterized by a general tendency for the velocity to decrease with depth and the tendency is occasionally overwhelmed (at about 27 and 52 km depth) by rapid velocity changes perhaps associated with phase or compositional changes. 相似文献
11.
A. I. Opara C. C. Agoha C. N. Okereke U. P. Adiela C. N. Onwubuariri J. O. Okpono O. P. Nosiri 《Journal of the Geological Society of India》2017,90(2):187-195
The problems of poor data quality and statics in seismic surveys have been attributed to lack of proper understanding of the low velocity layer characteristics of the area from which such data was acquired. Downhole seismic refraction survey was therefore conducted at twenty (20) borehole locations within parts of Niger Delta, Nigeria to determine the low velocity layer characteristics of the area using the Geometrics Stratavisor NZ11 instrument. The data was processed using Udysys software with spatial representation of the results presented. Static corrections were carried out on reflection seismic data acquired from the study area using Geoscribe II software to determine the effects of the low velocity layer on reflection seismic data in the area. Results of the study revealed that the velocity of the low velocity layer ranged between 144 and 996m/s with a regional average of 407m/s. The thickness of the low velocity layer varied between 3.0 and 9.6m with a mean value of 5.0m. Similarly, the velocity of the consolidated layer ranged between 1449 and 1812m/s with a mean value of 1738m/s. Results of the static correction carried out on the seismic reflection data revealed a substantial improvement in the resolution of the data after static correction. Based on these findings, it is therefore, recommended that shots for reflection seismic survey should be located at a minimum depth of 9.6m in the area to eliminate the effects associated with the low velocity layer. 相似文献
12.
上海地区场地剪切波速的特征分析 总被引：8，自引：0，他引：8
通过对上海地区场地剪切波速资料的统计分析,较深入地探讨了上海地区场地剪切波速在100m深度内的分布范围及其变化规律,可在工程实践中参考使用。 相似文献
13.
地壳校正在长江中下游地区远震层析成像中的应用 总被引：1，自引：0，他引：1
利用布设在长江中下游地区的47个固定台站所接收到的473个远震事件,对该地区进行了地壳校正研究。结果显示：(1)内陆地区下方的地壳呈现为低速异常,而沿海地区下方的地壳却呈现为高速异常;(2)地壳校正前后的速度异常确有变化,但差别不是很大,说明长江中下游地区的地壳结构比较稳定;(3)随着深度的增加,速度异常的差别越来越小,说明地壳校正对浅部的速度结构影响较大,而对深部的影响较小。因此,在远震层析成像研究中,若缺少浅部信息,可以进行地壳校正,以消除或减少地壳结构对最终反演结果的影响,从而提高深部结果的质量。 相似文献
14.
推导了基于角度域共成像点道集的叠前深度偏移层析速度分析公式,提出一种共散射点（CSP）道集与角道集串级优化叠前偏移的速度分析方法。该方法通过基于CSP道集的叠前时间偏移速度分析获取初始速度,利用基于角度域共成像点道集（ADCIGs）的叠前深度偏移速度分析进行速度更新。实现步骤概括为：将叠前地震数据映射为CSP道集,利用CSP道集叠加速度谱拾取能量团获取均方根（RMS）速度场;通过Dix公式将RMS速度转换为层速度作为层析的初始输入速度,基于ADCIGs实现叠前深度偏移层析速度反演,最终得到高精度的叠前偏移速度场。断层模型和实际资料试算结果验证了该方法的正确性和有效性。 相似文献
15.
Claus Prodehl 《Tectonophysics》1985,111(3-4)
In February 1978 seismic-refraction profiles were recorded by the U.S. Geological Survey along a 1000 km line across the Arabian Shield in western Saudi Arabia. This report presents a traveltime and relative amplitude study in the form of velocity-depth functions for each individual profile assuming horizontally flat layering. The corresponding cross section of the lithosphere showing lines of equal velocity reaches to a depth of 60–80 km.The crust thickens abruptly from 15 km beneath the Red Sea Rift to about 40 km beneath the Arabian Shield. The upper crust of the western Arabian Shield yields relatively high-velocity material at about 10 km depth underlain by velocity inversions, while the upper crust of the eastern Shield is relatively uniform. The lower crust with a velocity of about 7 km/s is underlain by a transitional crust-mantle boundary. For the lower lithosphere beneath 40 km depth the data indicate the existence of a laterally discontinuous lamellar structure where high-velocity zones are intermixed with zones of lower velocities. Beneath the crust-mantle boundary of the Red Sea rift most probably strong velocity inversions exist. Here, the data do not allow a detailed modelling, velocities as low as 6.0 km/s seem to be encountered between 25 and 44 km depth. 相似文献
16.
水利部松辽委黑龙江水文水资源勘测局、黑龙江省水文局和美国SonTek／YSI水文仪器公司合作，在黑龙江黑河地段的卡伦山水文站进行了冰期流量、流速和水深的比测研究。比测研究采用了SonTek／YSI的1．5MHz河猫Mini—ADP进行实测，并与先期采用机械式旋杯流速仪的实测资料进行比对。比测研究的目的是通过声学多普勒定点测流技术与标准的机械流速仪测量技术进行对比，验证声学多普勒剖面流速仪定点流量测量的精度，推广应用声学多普勒测流技术在封冰期测流的方法。 相似文献
17.
The existence of the upper mantle low velocity layer (LVL) below 100 km depth in cratonic areas is tested with surface waves dispersion curves. Given the ambient noise we find that a pronounced LVL (80 km thick and 2% velocity reduction or 40 km thick and 5% velocity reduction) can be distinguished from a constant velocity model by comparison of the fundamental mode group velocities, whereas a thin LVL (less than 40 km thick) with small velocity contrast (less than 2%) cannot be resolved. The fundamental modes of Love and Rayleigh waves have similar properties and, in general, the phase velocity differences are smaller than the standard error. Phase velocity alone cannot discriminate between the models, and the group velocity is in general more sensitive to the velocity structure than the phase velocity. The higher modes at short periods could potentially determine a LVL but in reality it is difficult to obtain sufficiently accurate measurements. We invert the synthetic dispersion curves by the non-linear Hedgehog inversion method. A pronounced LVL (more than 40 km thick and with a strong velocity contrast of about 5%) is detectable by the non-linear inversion but for a thin LVL with a strong velocity contrast it is not possible to resolve both velocity and thickness. In the inversions all solutions include a LVL for models with a pronounced LVL, whereas the solution space includes models with and without a LVL for models with a zero or positive gradient velocity–depth structure.We invert also real data with travel path across the Siberian craton with the Hedgehog method. Almost all solutions include a LVL in the depth range of 80–150 km with a velocity contrast up to 2% to the surrounding intervals. Hence, the LVL appears to be a common feature of the Siberian upper mantle, although a constant velocity at the same depth range cannot be totally excluded. Despite low resolution at large depth, a pronounced asthenospheric LVL below a depth of about 225 km is a constant characteristic of the set of solutions. 相似文献
18.
The Karous and Hjelt filter has been long time used as a qualitative interpretation of VLF-EM data. It is derived directly from the concept of magnetic fields associated with the current flow in the subsurface and resulted in a 2-D cross section showing the current density distribution at different depths. Practically, as the distance between measuring points increases, the total depth of the 2-D current density distribution section increases. Theoretically, the common guide to estimate the depth of penetration of an electromagnetic wave is the skin depth, which depends on the frequency of the electromagnetic wave and the conductivity of the host geological material, regardless of the distance interval between measuring points. Accordingly, the accuracy of the Karous and Hjelt filter regarding depth estimation of the anomaly is tested in this study. We proposed a conductive anomaly in a definite dimension and depth. The response of this conductive body is calculated as in-phase and out-of-phase synthetic VLF data via forward modeling. The synthetic VLF data is filtered by the Karous and Hjelt filter at 1, 5, and10 m of interval distance between measuring points. The present study showed that the Karous and Hjelt filter is characterized by a large degree of accuracy in depth estimation. 相似文献
19.
波流作用于海床产生动态孔隙水压力,如不能及时消除会在其内部产生累积孔隙水压力,相邻两点间的孔隙水压力差值造成的水力梯度产生渗流力,渗流力引起水流动,海床表面为排水界面,从而会在海床内部形成向上的渗流力作用于泥沙颗粒上,使泥沙发生启动向海床表层运移,从而形成一定范围的粗颗粒层。本文采用数值模拟对不同流速下的海床累积孔隙水压力进行了研究,同时分析了硬壳层的存在对海床累积孔隙水压力的影响规律,根据取得的不同流速下海床内部的累积孔隙水压力值,计算海床任意位置处的渗流压力梯度,采用王虎等(2014) 推导建立的海床临界冲刷深度的计算方法,分析不同流速下的硬壳层形成深度。结果表明: 海流流向与波浪行进方向一致时,对累积孔隙水压力起促进作用,流速越大累积孔隙水压力越大,反之对累积孔隙水压力有抑制作用。表面硬壳层的存在会显著促进累积孔压的消散,累积孔隙水压力沿深度分布的极值均出现在下层原始海床中,流速U0=0m ·s-1时硬壳层厚度由1m增加到3m,极值点深度下降了1.38m。累积孔隙水压力引起的渗流力对于海床泥沙启动影响显著,在流速U0=0m ·s-1,U0=1m ·s-1时泥沙启动深度均为海床1.5m深度处,并且海流流向与波浪行进方向一致时,会产生较大ΔP/ΔL值带动较粗的泥沙颗粒至海床表层,但对泥沙启动的最大深度影响不大。 相似文献
20.
Drakatos G. Melis N. Papanastassiou D. Karastathis V. Papadopoulos G.A. Stavrakakis G. 《Natural Hazards》2002,27(1-2):1-14
Three-dimensional velocity structure of the upper crust was determined by inversionof P-wave travel times in the region of Attiki Prefecture (Greece), located at the eastern part of the Greek mainland, which is traditionally considered as an area of low seismicity. An earthquake of Ms = 5.9 occurred there, on September 7, 1999, causing extensive damage in the metropolitan area of Athens. A two-step tomographic procedure was applied to investigate the 3-D crustal velocity structure. The data set consisted of travel time residuals of 466 very well located earthquakes. In order to improve the initial velocity model, before the inversion of the data, a `minimum 1-D' initial velocity model was obtained and, therefore, for the first time a reliable velocity model for the region was derived. Theresults show that the velocity distribution is influenced rather from the geology than the seismotectonic regime of the region. At shallow depths (less than 4 km) the velocity increases gradually with respect to the depth without any sharp variation. On the contrary, the lateral variation of velocity seems to be affected from the geological regime of the region. The low velocities at this depth seem to be typical for sedimentary basins, likethose of the investigated region. At deeper layers (larger than 5 km) a different picture is obtained where both the lateral and vertical velocity variations are sharply pronounced. At the depth of 8.5 km, the aftershock area is covered by relatively low velocities, while a region of higher velocity covers the central part of Attiki almost coinciding with the transition zone between the Pelagonian and Attico-Cycladic massifs. Finally, the influence of the geological regime is well expressed by a high velocity anomaly, which is predominant beneath the Palaeozoic and Mesozoic metamorphic basement of the investigated region. 相似文献