共查询到20条相似文献，搜索用时 906 毫秒
1.
本文推导并评价了一个新的计算视复电阻率的近似公式,其视振幅表达式为|ρs（ω）|≈ρs（ω）|ρs（ω）=ρs（ω）|,视相位表达式为φs（ω）≈sum from i=1 to n（Bi（ω）φi（ω））,这里Bi（ω）是按各介质复电阻率振幅计算的稀释系数。此近似公式比迄今为止已发表过的同类近似公式都精确,可在频率域激电法数值模拟计算视复电阻率时应用。 相似文献
2.
井中磁测在铁矿等磁性金属矿床勘查中具有举足轻重的作用.针对磁性金属矿床深部资源勘查中存在的有效信号弱、矿体形态复杂等技术难题,本文利用井中三分量磁测资料和地面磁测资料直接反演地下空间磁化率的分布情况,充分发挥纵、横向分辨率高的优势,通过磁化率的变化来确定矿（化）体的范围.分析了磁化率和磁场Hax、Hay、Za、ΔT各参量之间的关系,导出了磁化率反演方程;将钻孔编录、磁化率测井等结果作为约束条件构建了目标函数.以组合倾斜板状体模型为例,验证了方法的有效性,并在青海野马泉铁多金属矿区开展应用试验,试验结果与已有地质资料基本一致.该方法有效抑制了因反演数据源单一、缺乏约束条件而造成反演结果的多解性,实现了磁测资料的精细反演解释,为查明地下矿体空间位置、形态及规模,提高找矿效果,提供了一种新的解决方案. 相似文献
3.
本文分析了投弃式海流电场剖面仪的发展,简介了海流感生电场的基本原理,提出了投弃式海流电场剖面仪的技术方案.根据投弃式海流电场剖面仪的实际需求,研发了XCP海流电场传感器,并通过XCP探头的自旋转(16 r/s),实现了将海流电场信号AM调制并频移至海流电场传感器的超低噪声频段,解决了在高噪声背景下快速测量纳伏级微弱海流电场信号.设计实现了XCP探头前端弱信号处理电路,对海流电场微弱信号进行滤波提取的同时可实现对海流电场同向分量进行硬件电路补偿,在一定程度上克服了XCP探头下沉引起感生电场的强干扰.在XCP探头内部采用SoPC技术实现对海流电场信号、罗盘线圈信号和温度信息的快速测量及其数字化处理,并将数字信息以UART协议及LVDS物理层数传方式发送到XCP浮筒端.开创了长度2 km、直径0.1 mm漆包线动态数据传输技术,解决了XCP探头和XCP浮筒之间的数字化数据传输问题.根据XCP探头所采集的海流电场信号与罗盘线圈信号的同相分量In、正交分量Qn、基线量Bn数据,研究了XCP探测方法,从而计算出了海流的东向与北向相对速度分量VEr、VNr.采用所研发的XCP,在我国南海海域首次采集到海面至海下千米深度的XCP海流电场信息和海洋温度信息. 相似文献
4.
自然电场法常用于环境与工程等领域的监测作业,但各时刻观测数据往往单独反演解释.为了充分利用时序数据间的关联信息,提高监测数据的反演解释可靠性,提出基于卡尔曼滤波的自然电场监测数据时序反演方法.根据达西定律和阿尔奇公式建立污染物在孔隙介质中的运动扩散的动态地电模型,作为用于构建卡尔曼滤波的状态模型.而卡尔曼滤波的观测模型则通过常规的自然电场法正演获得.在建立状态模型和观测模型的基础上,构建起卡尔曼滤波递归,将地电模型演化信息与自然电场观测数据进行信息融合,实现自然电场监测数据的时序反演.加入噪声的自然电场模拟数据测试表明时序反演算法具有较好的鲁棒性,对噪声不敏感.沙槽物理实验监测数据的计算测试也同样证明时序反演能有效处理监测数据,实现对动态模型的准确重构. 相似文献
5.
利用虚磁荷的概念作磁场向上延拓,首先是提出的。他研究了地形水平的情况.设观测面上某点Q（α,β,γ）的单位面积虚磁荷的量为 m=Za（α,β,γ）/2π. （1）Za（α,β,γ）为Q（α,β,γ）点实测的垂直磁异常,则向观测面上半空间任一点P（x,y,z）延拓的公式为 相似文献
6.
可控源音频大地电磁法(CSAMT)一直沿用大地电磁法(MT)的办法,通过计算电场分量与磁场分量的比值,求取卡尼亚视电阻率.而CSAMT场源已知,电场分量和磁场分量都与地下电阻率存在一定的关系,可以单独采用CSAMT电场分量或者磁场分量提取地下介质的视电阻率.本文通过分析电场分量与磁场分量的数据特性,提出利用CSAMT电场单分量数据进行视电阻率的计算,用改进的广义逆矩阵反演方法,使初始模型中的地电层数等于频道个数,克服了以往反演计算中层数较少的问题;实现全场区电场分量视电阻率曲线的拟合反演.同时对单分量视相位计算方法进行分析,结合山西大同地区积水采空区探测及数据解释结果,论证本文提出的单分量解释方法的有效性. 相似文献
7.
结合地面电性源瞬变电磁法（TEM）探测深度大和地-井TEM探测精度高的优点,本文提出对电性源地-井TEM进行研究.基于一维正演理论,本文对电性源在地下激发的六个电磁场分量的扩散、分布特性和探测能力进行分析研究.研究结果表明地下瞬变场各分量的分布特征与地面情况类似,但是对地层的探测能力与地面情况存在较大差别.各分量的探测能力与它们的扩散特性有关,其中受积累电荷作用,垂直电场Ez和水平磁场Ḣx分量对目标层的反映最为明显,Ex和Ḣy分量在地下扩散时受"返回电流"的影响会出现变号现象,使得异常体带来的影响被掩盖,不易被分辨.本文研究结果为发展电性源地-井TEM的施工技术、数据处理与解释,建立了相应的理论基础,获得了对该方法的初步认识. 相似文献
8.
空中电场大地电磁法(Air Electric Field Magneto-Telluric method,简称AEMT),其基本的原理是,通过电容传感器测量近地表空中三个分量的交变电场,用磁棒观测交变磁场,再将所测电场和磁场转化为阻抗,通过对阻抗的解释,达到查明地下地质体的分布特征的目的.本文对AEMT基本原理进行较详细的论述,证明了电容传感器代替接电极原理的基本公式.分析了空气中垂直电场的来源,在介绍地面低频电磁波近似边界条件的基础上,导出了AEMT测量垂直电场分量时视电阻率的计算公式,并计算了一维情况下二层、三层地电模型AEMT视电阻率曲线.介绍了应用实例,最后讨论AEMT方法的技术特点. 相似文献
9.
本文讨论了行星际磁场B2分量变化时内磁层和中低纬度电离层的响应.指出B2变化引起的磁层大尺度对流电场的变化在一定条件下有可能透入内磁层,并沿磁力线映射到中低纬度电离层,在那里产生电场和电流体系,从而使Sq电流体系发生畸变,并在地面磁场中反映出来.数值计算表明,当△B2<0时,Sq电流体系的焦点向东和向高纬移动,地面磁场会观测到数伽马的变化.这就为中低纬地磁观测诊断磁层和太阳风状态提供了一种可能性.此外,本文还用上述物理过程解释了赤道地区一些高空物理现象,如B2倒转时电离层漂移速度的变化,赤道磁场异常以及赤道q型偶现E层的消失等等. 相似文献
10.
本文利用信使号飞船2011-2015年期间在轨磁场数据对水星磁尾电流片的磁场结构分布特征进行了统计分析.为探究磁场结构分布随水星径向距离的变化,电流片划分为近磁尾（-1.5RM > X > -2.0RM）和远磁尾（-2.0RM > X > -2.5RM）两个区域.所得结果表明：（1）无论是近磁尾还是远磁尾,电流片中的磁场都以+Bz分量为主,磁场方向几乎与磁赤道面垂直.（2）相比近磁尾,远磁尾电流片中磁场强度、Bz分量较弱,By分量较强,而且-Bz信号出现概率相对较大,这表明电流片中磁活动相对容易在远磁尾中发生.（3）磁场强度以及Bz分量在晨昏方向上的分布存在晨昏不对称性——在方位角120°~190°范围内相对较弱.弱Bz数据点（Bz<5 nT）也在昏侧（Y>0）发生较为频繁.（4）与Bz分布相反,磁场强By分量（|By|>5 nT）倾向于在晨侧（Y<0）发生.统计分析还表明,磁场By分量与行星际磁场By分量并无明显的相关性.对比地球磁尾电流片,我们对水星磁尾电流片Bz分量、强By分量的晨昏不对称起源机制作了探讨分析. 相似文献
11.
Umesh C. Das 《Geophysical Prospecting》1995,43(3):417-432
We consider the calculation of the electrical field quantities, electric potential and the vertical component of the total volume density of electric current, in a horizontally layered, piecewise homogeneous and arbitrarily anisotropic earth due to a system of direct current point sources. By applying Fourier transformation with respect to the horizontal space coordinates to the static field equations, the field quantities are obtained as the solutions of the system of transform-domain differential equations in the vertical (depth) coordinates. A recurrence scheme has been given to compute the tranform-domain field quantities at any depth. The corresponding space-domain quantities are then obtained by inverse Fast Fourier Transformation (FFT). A complete computer program has been developed for computing the electric potentials at any depth of the layered earth, which is composed of an arbitrary number of anisotropic layers with arbitrary conductivity tensors. By considering the point sources at different depths from the surface, equipotential contours on the surface of arbitrarily anisotropic layered earth models are given. 相似文献
12.
The fine structure is discussed arising in the spatial distribution of the pulsed electric field above a Γ-shaped stroke of lightning. The channel of discharge contains a vertical and a horizontal section. The structured spatial distribution of field appears due to a superposition of three pulses arriving from vertical and horizontal sections of the causative discharge and from reflections from the ground. The details of electric field distribution depend on time and on the stroke orientation relative to an elevated observer. The characteristic size of ‘filaments’ in the transient electric field is about 1 km along the horizontal direction, while it reaches a few tens of kilometers along the vertical direction. 相似文献
13.
强地震会造成电离层电场发生异常变化.基于大气层-电离层电动力学理论对地震电离层异常电场开展数值模拟和研究,将理论推导出来的电离层异常电场方程扩展到球面坐标系中,并且考虑到电离层层电导率的各向异性,建立新的地震电离层异常电场模式.引进一个电离层层电导率经验公式(Nopper and Carovillano,1979),对中低纬度地震电离层异常电场特性进行数值模拟.模拟结果表明:附加电流引起电离层异常电场范围远大于自身在地表上的分布.且发生在低纬地区的异常电场主要成分是纬向电场,在东西两侧显偶极子分布.在额外电流分布相同的情况下,夜晚生成的异常电场更显著,存在昼夜差异. 相似文献
14.
Charged particle motion in magnetoactive plasma with an axially symmetric electrostatic field has been studied. It has been indicated that a difference between drift velocities of electrons and ions leads to a magnetic field disturbance. The equations for stationary magnetic field disturbances stretched along the magnetic field, which can be magnetic ducts for propagation of whistlers, have been obtained. The possibility of formation of such ducts by electrostatic fields from thunderstorm sources, penetrating into the ionosphere, has been estimated. 相似文献
15.
江苏地区地电场变化特征与差异性分析 总被引：1，自引：0，他引：1
处理、分析了江苏省4个台的地电场日变化资料,结合地磁场水平分量H、线应变理论固体潮,研究了地电场日变化特征和差异,得到：（1）4个台地电场日变化明显,主要以12小时的半日波成分最强,8小时周期和全日波成分次之;（2）地电场日变化存在地磁场和固体潮影响。靠近海边及湖泊的台站,受固体潮的影响较为明显,各方向还具有明显的固体潮半月波,但没有像固体潮一样大小的波;而远离江、海、湖的一些台站观测到的地电场日变与地磁水平分量比较相关,其差异性与台站的位置、电性结构有关系。 相似文献
16.
L. J. TSAY 《Geophysical Prospecting》1976,24(1):70-78
A new scheme for continuing aeromagnetic data along a profile with constantly changing elevation to a horizontal level is presented in this paper. It only requires some modifications of the conventional methods which are designed to continue potential field data from one horizontal level to another level. The new scheme procedes in the following steps: (1) digitization of anomaly along flight level, thus giving distance and elevation to the desired horizontal level at each station. (2) upward continuation at each digitized point from the corresponding elevation to a desired horizontal level. The validity and usefulness of the scheme is shown with theoretical and real data. 相似文献
17.
Electromagnetic geophysical methods often rely on measurements of naturally occurring or artificially impressed electric fields. It is technically impossible, however, to measure the electric field directly. Instead, the electric field is approximated by recording the voltage difference between two electrodes and dividing the obtained voltage by the distance between the electrodes. Typically, modelling and inversion algorithms assume that the electric fields are obtained over infinitely short point-dipoles and thus measured fields are assigned to a single point between the electrodes. Such procedures imply several assumptions: (1) The electric field between the two electrodes is regarded as constant or being a potential field and (2) the receiver dimensions are negligible compared to the dimensions of the underlying modelling grid. While these conditions are often fulfilled for horizontal electric fields, borehole sensors for recordings of the vertical electric field have dimensions in the order of ≈100 m and span several modelling grid cells. Observations from such elongated borehole sensors can therefore only be interpreted properly if true receiver dimensions and variations of electrical conductivity along the receiver are considered. Here, we introduce a numerical solution to include the true receiver geometry into electromagnetic modelling schemes, which does not rely on such simplifying assumptions. The algorithm is flexible, independent of the chosen numerical method to solve Maxwell's equations and can easily be implemented in other electromagnetic modelling and inversion codes. We present conceptual modelling results for land-based controlled source electromagnetic scenarios and discuss consideration of true receiver geometries for a series of examples of horizontal and vertical electric field measurements. Comparison with Ez data measured in an observation borehole in a producing oil field shows the importance of both considering the true length of the receiver and also its orientation. We show that misalignment from the vertical axis as small as 0.1° may seriously distort the measured signal, as horizontal electric field components are mapped into the desired vertical component. Adequate inclusion of elongated receivers in modelling and inversion can also help reducing effects of static shift when interpreting (natural source) magnetotelluric data. 相似文献
18.
F. S. Mozer 《Pure and Applied Geophysics》1971,84(1):32-45
Summary Twenty-eight balloons have been flown in Canada to measure vertical and horizontal electric fields at balloon altitudes. A horizontal electric field of magnitude typically between 10 and 50 millivolts/meter has been measured at night at high latitudes in association with auroras and magnetic disturbances. Its origin is in the magnetosphere and it maps to balloon alitudes with small attenuation according to Maxwell's equations. The vertical electric field at the balloon displays variations as the horizontal ionospheric field changes in order to maintain
. Thus, magnetospheric processes affect both vertical and horizontal atmospheric electric fields and the potential differences induced by these processes may be comparable to weather induced potential differences. Weather processes have also been observed to produce large horizontal electric fields at balloon altitudes. Methods of distinguishing horizontal fields of ionospheric origin from those of weather origin are investigated with the conclusion that a determination of the source of a given event can often if not generally be made.This paper was presented byU. Fahleson 相似文献
19.