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61.
假定垂直轴为二维对称各向异性介质主轴之一,构造走向与另一主轴方向成任一夹角,用伽勒金(Galerkin)有限元法和矩形网格,优化地合成总体刚度矩阵,使二维各向异性介质的基本方程形成有限元代数方程组,求出各节点场值,并利用MOM法求出辅助场,进而求出张量阻抗等响应函数.同时还对有关文献的计算模型进行了数值模拟检验 相似文献
62.
为详细了解崇明越江通道南港隧道段地层情况 ,设计要求提供长江水域静探资料。简介了我院水域静力触探设备的研制和应用情况 相似文献
63.
高密度电法勘察岩土工程实例 总被引:6,自引:1,他引:6
利用岩土层间的导电性差异特性,使用由WDJD-1型主机与WDZJ-1多路电极转换器组成的高密度电法测量系统,按照不同的工程要求,采取不同的排列方式进行勘探,并用RES2DINV(演示版)高密度电阻率数据二维反演软件对所采集的数据处理解释,可实现对不同岩土层界面的划分。与常规电法相比,其方法手段更为先进,定性定量解释可靠,影像图件直观清晰。 相似文献
64.
Dense profile-oriented resistivity data allows for 2D and 3D inversions. However, huge amounts of data make it practically impossible to do full 2D or 3D inversions on a routine basis. Therefore, a number of approximations have been suggested over the years to speed up computations. We suggest using a combination of Broyden's update on the Jacobian matrix with derivatives calculated using a 1D formulation on a parameterized 2D model of locally 1D layered models. The approximations bring down the effective number of 2D forward responses to a minimum, which again gives us the ability to invert very large sections. Broyden's update is not as useful with a parameterized problem as is the case with a smooth minimum structure problem that has been the usual application. 1D derivatives, however, seem to be very effective when initiating a full 2D solution with Broyden's update. We compare the different methods using two different kinds of data on two synthetic models and on two field examples. The most effective and reliable optimization combines 1D derivatives with a full 2D solution and Broyden's update. When using Broyden's update the Jacobian matrix needs to be reset every once in a while. We do this whenever the difference in data residual from the previous iteration is less than 5%. This combined inversion method reduces the computation time approximately a factor of 3 without losing model resolution. 相似文献
65.
This study investigates an electric‐type active mass driver (AMD) system for structural vibration control. Composed primarily of an electric servomotor and a ball screw, the electrical AMD system is free from noise problems, oil leakage, and labor‐intensive maintenance that commonly are associated with hydraulic AMD systems. The desired stroke amplification of the mass and the power demand of the servomotor can be adjusted via the ball screw pitch, which in turn affects the effectiveness and efficiency of the system. Meanwhile, an instantaneous optimal direct output feedback control algorithm is adopted. Numerical simulation is performed using a five‐story steel frame as the object structure under the conditions of the 1940 El Centro earthquake. The AMD system proves to be effective and efficient within a certain range of the ball screw pitch. The reductions of the peak responses can reach as high as 70% if properly designed. Requiring only the velocity measurement of the top floor for on‐line feedback control, the proposed control algorithm is recommended for practical implementation. Copyright © 2004 John Wiley & Sons, Ltd. 相似文献
66.
基于电场理论的主动防雷系统的初步设想 总被引:1,自引:0,他引:1
针对目前使用的传统雷电防护技术存在的问题,通过分析雷电原理和雷电触发机制,利用电场理论来设计一套主动防雷系统,即实现保护对象所在空间大气处于被激放电状态,并利用闪电将大气激活为自激放电状态。介绍了主动防雷系统的原理,并对其核心的“引而不发”理论进行阐述,在此基础上设计出主动防雷系统的模型。具体说明了构成主动防雷系统的阻塞系统、疏导系统和电源系统的构造和特征以及它们之间的关系。计算得到主动防雷系统所需的电场强度E=0.69kV/m。最后指出了存在问题与发展方向,在结论中总结了主动防雷系统的特点及其关键。 相似文献
67.
68.
通过对我国主要金矿类型中黄铁矿导电类型的分析表明,黄铁矿“电子。空穴心”与金矿床的成因类型具有密切的联系,华北地台太古代变基性火山岩中的金矿床(绿岩带型)、热水淋滤型(卡林型)金矿床,黄铁矿多为单一的“电子心”型导电。大多数产于中生代岩体中的中深脉状金矿、火山次火山岩中的金矿床,黄铁矿为“电子心”、“空穴心”混合型导电,个别的为单一的“空穴心”导电。黄铁矿的“电子.空穴心”受杂质成分As、Co、Nl在成矿背景中的丰度,进入黄铁矿品格中的替代能力的差异、补偿类质同象现象、成矿时温度以及.f(S2)等多种因素的耦合制约。 相似文献
69.
S. V. Bogdanova I. K. Pashkevich V. B. Buryanov I. B. Makarenko M. I. Orlyuk V. M. Skobelev V. I. Starostenko O. V. Legostaeva 《Tectonophysics》2004,381(1-4):5
The deep structure of the gabbro–anorthosite–rapakivi granite (“AMCG-type”) Korosten Pluton (KP) in the northwestern Ukrainian Shield was studied by 3-D modelling of the gravity and magnetic fields together with previous seismic data. The KP occupies an area of ca. 12,500 km2 and comprises several layered gabbro-anorthositic intrusions enveloped by large volumes of rapakivi-type granitoids. Between 1.80 and 1.74 Ga, the emplacement of mafic and associated granitoid melts took place in several pulses. The 3-D geophysical reconstruction included: (a) modelling of the density distribution in the crust using the observed Bouguer anomaly field constrained by seismic data on Moho depth, and (b) modelling of the magnetic anomaly field in order to outline rock domains of various magnetisation, size and shape in the upper and lower crust. The density modelling was referred to three depth levels of 0 to 5, 5 to 18, and 18 km to Moho, respectively. The 3-D reconstruction demonstrates close links between the subsurface geology of the KP and the structure of the lower crust. The existence of a non-magnetic body with anomalously high seismic velocity and density is documented. Most plausibly, it represents a gabbroic stock (a parent magma chamber) with a vertical extent of ca. 20 km, penetrating the entire lower crust. This stock has a half-cylindrical shape and a diameter of ca. 90 km. It appears to be connected with a crust–mantle transitional lens previously discovered by EUROBRIDGE seismic profiling. The position of the stock relative to the subsurface outlines of the KP is somewhat asymmetric. This may be due to a connection between the magmatism and sets of opposite-dipping faults initially developed during late Palaeoproterozoic collisional deformation in the Sarmatian crustal segment. Continuing movements and disturbances of the upper mantle and the lower crust during post-collisional tectonic events between 1.80 and 1.74 Ga may account for the long-lived, recurrent AMCG magmatism. 相似文献
70.