埋设地下光缆对武都地电影响的分析   总被引：3，自引：0，他引：3       下载免费PDF全文

高曙德  严正  康好林  苏永刚 《地震工程学报》1999,21(4):433-435

着重探讨武都地电台测区埋设地下光缆后北西道地电阻率测值急剧上升的原因.通过实际观测、理论分析和实验,总结出了这种变化的机制,定量地解释了埋设地下光缆对地电观测的影响,从而为以后判断地电测值变化是干扰还是地震异常提供了依据.  相似文献   

西藏当雄地区构造地貌及形成演化过程   总被引：8，自引：2，他引：8  

吴珍汉  胡道功  刘崎胜  夏浩东  鄢犀利 《地球学报》2002,23(5):423-428

西藏当雄地区在区域性挤压缩短期后发育2种典型层状地貌面，即山顶面与盆地面，不同地块具有不同特点与不同高度的山顶面。山顶面形态与分区性、分段性明显受早期逆冲推覆构造与晚期断裂所控制，山顶面梯级带对应于区域张性－张扭性断裂与盆－山构造－地貌边界。原始山项面或高原主夷平面主要形成于15－8Ma，念青唐古拉山脉开始快速隆升与两侧地块初始断陷时代为8－4Ma，羊八井－当雄－谷露盆地快速裂陷事件发生于2－1．5Ma,区域NW向走滑断裂与现今河流峡谷主要形成于1．4Ma以来。当雄及邻区层状地貌面的形成、裂解与演化良好地反映了青藏高原腹地挤压缩短与地壳增厚期后区域构造活动和地貌环境变迁的动力学过程。  相似文献   

Vening—Meinesz公式的球面卷积形式   总被引：4，自引：0，他引：4  

宁津生  晁定波 《测绘学报》1994,23(3):161-166

过去利用快速Fourier变换（FFT）或快速Hartley变换（FHT）技术计算垂线偏差是假设地球是一个平面。在此基础上导出的Vening-Meinesz公式平面卷积形式虽然在一定精度范围内可以满足要求，但会产生较大的近似误差。然而，Vening-Meinesz公式同样可以发展为由FHT技术计算的二维球面卷积公式。数值计算表明：在Δ(?)=10°，Δλ=13°（5′×5′平均重力异常）范围内，Vening-Meinesz球面卷积公式的计算结果与数值积分结果的均方差m_ξ=±0.03秒、m_η=±0.02秒，比平面卷积公式的计算结果与数值积分结果的均方差m_ξ=±0.14秒、m_η=±0.30秒有显著提高。  相似文献   

利用二维DLT及光束法平差进行数字摄像机标定   总被引：34，自引：5，他引：34  

张永军  张祖勋  张剑清 《武汉大学学报(信息科学版)》2002,27(6):566-571

利用共线方程和二维DLT之间的对应关系导出了由二维DLT的8个参数表达的主纵线方程式，讨论了主点初值和求解方法，给出了单张像片摄像机参数分解不惟一性及临界序列的证明，详细推导了利用二维DLT参数分解摄像机外方位元素初值的实用算法，论述了利用光束法平差进行摄像机标定的数学模型，实际图像数据实验取得了很好的结果，验证了本文所提出的摄像机标定算法的可行性。  相似文献   

平面相控阵脉冲压缩的雷达气象方程     

张子良  郑国光  葛文忠  魏鸣 《南京气象学院学报》2013,5(5):426-431

在低发射功率条件下,相控阵多普勒天气雷达为了增加探测距离和提高分辨率,需要采用脉冲压缩技术.由于采用相控阵技术,波束扫描过程中,在平面阵非法线方向上会产生波束展宽,引起波束内功率下降,需要在计算雷达气象方程时弥补功率下降的误差.平面相控阵天气雷达在探测远距离目标时,使用宽脉冲发射,经脉冲压缩处理以提高分辨率,因此需要建立适用的雷达气象方程.首先讨论了脉冲压缩低峰值功率的平面相控阵多普勒天气雷达的结构、线性调频脉冲压缩的距离(多普勒测量)、调频波形的耦合问题以及目标距离的测量;然后给出了适用于脉冲压缩的平面相控阵雷达气象方程,此方程同时也适用于一维线性阵的脉冲压缩的天气雷达.  相似文献   

Alluvial stratification styles in a large,flash‐flood influenced dryland river: The Luni River,Thar Desert,north‐west India     

Paul A. Carling  Suzanne F. Leclair 《Sedimentology》2019,66(1):102-128

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Breaching-related turbidites in fluvial and estuarine channels: Examples from outcrop and core and implications to reservoir models     

《Marine and Petroleum Geology》2017

An understanding of the paleoenvironment and the main sedimentary processes behind preserved deposits is crucial to correctly interpret and represent lithofacies and facies associations in geomodels that are used in the hydrocarbon industry, particularly when a limited dataset of cores is available. In this paper a fairly common facies association is discussed containing massive sands - here defined as thick (>0.5 m) structureless sand beds devoid of primary sedimentary structures, or with some faint lamination - deposited by mass failures of channel banks in deep fluvial and estuarine channels. Amongst geologists it is generally accepted that liquefaction is the main trigger of large bank failures in sandy subaqueous slopes. However, evidence is mounting that for sand deposits a slow, retrogressive failure mechanism of a steep subaqueous slope, known as breaching, is the dominant process. A model of breaching-induced turbidity current erosion and sedimentation is presented that explains the presence of sheet-like massive sands and channel-like massive sands and the sedimentary structures of the related deposits. Sheet-like packages of spaced planar lamination that are found together with massive sand bodies in deposits of these environments are identified as proximal depositional elements of breach failure events. The model, acquired from sedimentary structures in deposits in the Eocene estuarine Vlierzele Sands, Belgium, is applied to outcrops of the Dinantian fluvial Fell Sandstone, England, and cores of the Tilje and Nansen fms (Lower Jurassic, Norwegian Continental Shelf). The possible breach failure origin of some other massive sands described in literature from various ancient shallow water environments is discussed. Breach failure generated massive sands possibly also form in deep marine settings. The potentially thick and homogeneous, well-sorted sand deposits bear good properties for hydrocarbon flow when found in such an environment. However, in case of deposition in an estuarine or fluvial channel, these sand bodies are spatially constricted and careful facies interpretation is key to identifying this. When constructing a static reservoir model, this needs to be considered both for in-place volume calculations as well as drainage strategies.  相似文献   

EXPERIMENTAL STUDY OF TEMPERATURE EVOLUTION AND IDENTIFICATION OF INSTABILITY POSITION OF PLANAR STRIKE-SLIP FAULT DURING PROCESS OF STICK-SLIP          下载免费PDF全文

REN Ya-qiong  MA Jin  LIU Pei-xun  CHEN Shun-yun 《地震地质》2016,38(1):65-76

Stick-slip of fault in laboratory accompanies change of temperature. Temperature change is not only concerned with sliding friction, but also with the stress state of the sample. In this article, we use infra-red thermal imaging system as wide-range observation means to study the temperature variation of different stages during the deformation of sample. The rock sample for the experiment is made of granodiorite from Fangshan County with a size of 300mm×300mm×50mm. It is cut obliquely at an angle of 45°, forming a planar fault. Two-direction servo-control system was used to apply load on the sample. The load in both directions was forced to 5MPa and maintained constant (5MPa) in the X direction, then the load in the Y direction was applied by a displacement rate of 0.5μm/s, 0.1μm/s and 0.05μm/s successively. The left and below lateral of the sample were fixed, and the right and top lateral of the sample were slidable when loaded. The experiment results show not only the temperature change from increase to decrease caused by conversion of stress accumulation to relaxation before and after the peak stress, but also opposite variation of temperature increase on fault and temperature decrease in rock during instability stage. Most important of all, we have found the temperature precursor identifying the position of instability through the temperature variation with time along the fault. It shows that rate of temperature increase of instability position keeps relative high value since the stage of strongly off-linear stage, and accelerates in stage of meta-instability. After separating the effect of friction and stress, we found that temperature increase occurs in the rock near the fault instead of on the fault, which means the mechanism of temperature increase is stress accumulation. Temperature of fault at the instability position does not increase, which means the position is locked. We speculate that the position of locked area on fault with high stress accumulation near the fault may be the future instability position. It is of significance of studying temperature variation during stick-slip to the monitoring of earthquake precursors. Heat caused by friction of earthquake needs long time to transfer to the surface and could not be detected as a precursor. While the stress of surface rock near the fault would change as the stress of interior rock changes, which could cause detectable temperature variations. The research purpose of this article is to find special change positions before instability. As the temperature variations are caused by stress and slip of fault, the results are also meaningful to analysis of stress and displacement data related to earthquake precursors.  相似文献   

Geology and age of the Glikson impact structure,Western Australia     

F. A. Macdonald  M. T. D. Wingate  K. Mitchell 《Australian Journal of Earth Sciences》2013,60(4-5):641-651

The Glikson structure is an aeromagnetic and structural anomaly located in the Little Sandy Desert of Western Australia (23°59'S, 121°34′E). Shatter cones and planar microstructures in quartz grains are present in a highly deformed central region, suggesting an impact origin. Circumferential shortening folds and chaotically disposed bedding define a 19 km-diameter area of deformation. Glikson is located in the northwestern Officer Basin in otherwise nearly flat-lying sandstone, siltstone and conglomerate of the Neoproterozoic Mundadjini Formation, intruded by dolerite sills. The structure would not have been detected if not for its strong ring-shaped aeromagnetic anomaly, which has a 10 km inner diameter and a 14 km outer diameter. We interpret the circular magnetic signature as the product of truncation and folding of mafic sills into a ring syncline. The sills most likely correlate with dolerites that intrude the Boondawari Formation ～25 km to the north, for which we report a SHRIMP U?–?Pb baddeleyite and zircon age of 508?±?5 Ma, providing a precise older limit for the impact event that formed the Glikson structure.  相似文献   

深度图像自动配准点云的方法研究     

田慧  周绍光  李浩 《测绘科学》2012,37(3):41-43

点云配准是三维激光扫描数据处理过程中不可或缺的一个环节,利用标靶进行配准是经典的手段之一,此类方案在单独扫描标靶的基础上进行半自动化配准。本文给出一种配准策略,利用中心投影原理将单站扫描的点云转换为深度影像,借助数字图像处理技术完成标靶的自动提取,拟合获得标靶中心点的坐标,并借用摄影测量学的知识实现点云的自动化配准。实验证明了本文方法的有效性。  相似文献