共查询到17条相似文献，搜索用时 765 毫秒
1.
井眼压力高于地层压力会导致泥浆侵入,电阻率测井响应受到泥浆侵入的影响而不能真正反映地层的电阻率特性。笔者依据双侧向电阻率测井的基本机理,气-水两相渗流方程及传导对流方程,进行仿真模拟,得到泥浆侵入高矿化度致密气层的二维轴对称模型。研究含水饱和度、地层电阻率以及深浅侧向井壁电场分布随侵入时间的变化规律。研究发现:随着侵入时间的增加,含水饱和度增大,地层电阻率减小;泥浆侵入对致密气层深浅侧向测井响应都产生一定的影响,导致致密气层深浅侧向电阻率幅度差比常规储层深浅侧向电阻率幅度差大,幅度差峰值出现较早。 相似文献
2.
稠油热采地层温度的独特变化规律直接影响了目的层和围岩的电阻率,进而导致阵列感应测井响应的变化;因此,了解地层温度对阵列感应测井响应的影响,对于更准确地确定地层电阻率具有重要的意义。本文利用地层温度与地层电阻率的相关关系,通过有限元方法模拟不同地层温度和不同地层结构的阵列感应测井响应。数值模拟结果表明：不同线圈结构子阵列的视电阻率随地层温度的升高而下降,下降幅度与地层温度、线圈系结构以及地层原始电阻率有关;三层阶跃地层中目的层及围岩电阻率、目的层温度和厚度都会影响其测井响应,使各子阵列视电阻率曲线由目的层边缘向围岩处呈现上升的形态。通过对这些响应特征的分析研究,结合油田实例G1井进行了对比和验证,模拟结果较好地阐释了现场阵列感应测井的异常响应特征。 相似文献
3.
火成岩中网状裂缝双侧向测井响应特征 总被引：3，自引：1，他引：2
针对海拉尔布达特储层的实际情况,利用基于电阻网的有限差分模拟方法,分别计算了一组平行缝、两组平行缝呈不同夹角和泥浆沿网状缝入侵情况下的双侧向测井响应。总结出网状裂缝发育火成岩储层双侧向测井响应特征：一组高角度平行裂缝使双侧向幅度呈现正幅度差,低角度裂缝呈现负幅度差,低角度裂缝电阻率降低更多;构成网状裂缝的两组平行裂缝的倾角和夹角同时影响双侧向测井响应,当两组裂缝夹角较小时,双侧向幅值特征趋向于一组平行缝的情形,而随着夹角增大,电阻率幅度降低,倾角影响变小;泥浆侵入带的存在除了造成双侧向曲线明显的正幅度差外,还使裂缝倾角和夹角的影响变模糊。该结果将为火成岩裂缝储层的识别和评价提供理论依据。 相似文献
4.
《物探化探计算技术》2016,(1)
几何因子对于计算地层真实电阻率、了解地层特性、划分储层等起着相当重要的作用。这里建立双线圈系感应测井基本模型,分别得出纵、径向简单多层地层模型的几何因子理论曲线,从中可得知感应测井响应值受到目的层厚度、围岩电阻率、泥浆电阻率、侵入带等多种情况的因素影响,1目的层越厚,感应测井值越接近原状地层电阻率值;2在过渡带厚度不变的情况下,冲洗带深度越大,测量的电阻率越小,它的径向几何因子有下降的趋势,但是整体来说,随着冲洗带的半径增加,视电导率增加幅度变缓,且越来越接近过渡带地层的电导率;3在冲洗带厚度不变的情况下,过渡带的深度越小,越接近原始地层的电导率;4泥浆侵入会导致得到的地层电阻率与实际地层电阻率存在较大偏差。将这些结论应用于计算塔河油田石炭系区域井的真实电阻率中,得到塔河油田石炭系区域地层电阻率真值,最后解释结果与试油结果对比证实,这一过程确实提高了地层电阻率和冲洗带电阻率的精度。 相似文献
5.
CHEN Qi-yan FAN Xiao-min College of GeoExploration Science Technology Jilin University Changchun China 《吉林大学学报(地球科学版)》2006,(Z2)
由于泥浆滤液、地层非均质性等各种因素综合影响,同一地层的侵入带半径也常常不是恒定的,而是随深度而变化基于趋肤效应几何因子理论,论述了倾斜侵入带前缘的正演计算理论和方法,分析了不同侵入深度及侵入带前缘与井轴方向不同夹角的感应测井响应特征。结果表明,侵入带形状对测井曲线的幅度和形状影响很大,为解释侵入带环境对测井结果的一般影响和一些测井异常提供了理论依据,应该在测井解释工作中注意该项影响。 相似文献
6.
泥浆滤液侵入渗透性地层会改变井周地层流体的原始分布状态,使井周地层电阻率发生变化、储集层电测井响应失真。本文基于油水两相渗流理论和水对流扩散理论,应用数值模拟方法构建地层模型,研究低渗储层泥浆侵入过程中井周地层矿化度、含水饱和度、电阻率变化特征及井周油藏分布特征。对不同渗透率地层泥浆侵入的数值模拟结果表明:在低渗透储层,相同侵入时间内,随着地层渗透率的增加,泥浆侵入深度增加,且同一侵入深度的含油饱和度减小;随着侵入时间的增加,井周地层水矿化度、含水饱和度和地层电阻率的侵入剖面前缘均发生明显的变化。结合3口井的泥浆侵入数值模拟分析,发现阵列感应测井响应特征及其电阻率的幅度差异受泥浆侵入时间和侵入深度影响。不同流体性质层段的井周油藏动态演化规律模拟结果表明,井周油藏的变化情况与储层流体性质有明显关系。利用实例井侵入模拟结果与阵列感应测井响应的相关性,构建了侵入深度的计算公式;根据侵入阶跃剖面,利用几何因子理论构建了原始地层电阻率计算公式,用以辅助储层电阻率校正。正确认识井周地层泥浆侵入特征及井周油藏的分布情况有助于提高阵列感应测井评价储层的准确性。 相似文献
7.
8.
自然电位测井数值计算中的激励源分布 总被引：1，自引：0，他引：1
为实现自然电位测井的高效正演计算,以定量研究各种因素影响,针对自然电位的激励源-偶电层的分布进行了研究。通过对自然电位产生原因及偶电层对自然电位贡献的分析,认为只有泥岩井壁、侵入带中砂泥岩界面和侵入带与原状地层分界面处的偶电层对自然电位测井值有贡献,而研究砂岩层处的自然电位异常,则仅考虑由侵入带与原状地层界面处的偶电层即可。通过直流电场与静电场的类比,推出了偶极源的面电流密度表达式,并通过计算研究了均匀介质中侵入深度的影响。结果显示,自然电位曲线形状随侵入深度增加而变得平缓,异常幅度减小。 相似文献
9.
不同井眼条件下的水平井双侧向测井响应 总被引：1，自引：0，他引：1
为解决油气开发中水平井中井眼对双侧向测井响应的影响,建立了上、中、下三层介质的水平井模型,采用三维有限元方法进行研究。数值计算结果表明,水平井眼处于目的层不同位置、不同井眼尺寸以及泥浆电阻率等都对水平井双侧向测井响应有不同程度的影响,特别是对非厚层影响更加明显。井眼尺寸越大和泥浆电阻率越高,对双侧向测井响应的影响就越严重。当目的层小于6 m时,水平井中的深、浅双侧向测井响应都不同程度地受到层厚围岩的影响;当层厚分别大于36 m和6 m时,深侧向和浅侧向测井几乎不受围岩影响;在15°的范围内,不同的井眼倾角对双侧向测井响应影响不大。 相似文献
10.
为了准确划分直罗组地层岩性、识别地层及解译矿层,通过综合分析鄂尔多斯盆地4个主要铀矿集区侏罗系直罗组地层的定量伽马、自然电位、三侧向电阻率、密度4条测井曲线参数,采用归类统计和测井曲线形态分析,结果显示不同地区直罗组的伽马照射量率数值差异不大,东南缘地区电阻率值明显高于其他地区,密度值变化呈现"南高北低"特征;垂向上直罗组上段的伽马背景值和电阻率相对直罗组下段偏低,密度值变化不大;区域上直罗组地层中从粗砂岩到泥岩的伽玛背景值逐渐增高;密度值略微增高,电阻率和自然电位异常幅度由大变小。根据不同类型岩石测井参数和相系差异,建立了东北缘地区电阻率与密度交会图版岩性识别模型。煤田钻孔测井岩性解译时具有放射性异常的砂岩段粒度应提高1~2个级别。 相似文献
11.
We suggest to approximate the depth-dependent conductivity of layered formations by continuous functions and use this approach to design an algorithm for 2D inversion of induction logging data. The logs represent formations consisting of alternating thin clay and sand layers of varying thickness, in which the sand layers can involve a developed invaded zone of a complex structure. Comparison of synthetic logs in models with piecewise constant and continuous approximations of conductivity shows that the continuous-function approximation is accurate within 5%, and the accuracy improves as the average conductivity of the layered formation is taken into account. 相似文献
12.
《Russian Geology and Geophysics》2014,55(5-6):775-783
Coupled geomechanic and fluid flow analysis is applied to develop theoretical and experimental background for geosteering and well logging to diagnose the state of near-wellbore formation and oil reservoir. The suggested methods of processing EM induction (VIKIZ) and Russian laterolog (RLL) resistivity responses account for effects of stress-dependent fluid flow changes. The geomechanic and fluid-flow effects on resistivity well logs are investigated for the case of asymmetric invasion and related irreversible deformation. Ways of taking into account stress-dependent effects on resistivity logs are developed on the basis of 3D modeling of geomechanic and electromagnetic fields. 相似文献
13.
贵州省罗甸透闪石矿床地质特征及找矿预测 总被引：1，自引：0，他引：1
罗甸透闪石矿床属燕山期岩浆热液矿床,成矿作用为接触交代;侵入岩体为辉绿岩,属偏碱性基性幔源浅成岩,岩体呈似层状顺层侵入于二叠系中统栖霞组（P2q）与茅口组（P2m）接触面之间;围岩蚀变有透闪石化和大理岩化,由岩体向外依次分为大理岩化带→透闪石化带;软玉矿体赋存于外接触带茅口组一侧,顺层产出;含矿带厚10～30余米,其中夹矿体十余层,矿体形态以似层状为主,次为透镜状,厚0.05～0.3 m。在1000 km2范围内发现5个辉绿岩体露头,呈带状出露,长3～35 km,显示有矿化,具有较好的找矿远景。 相似文献
14.
井资料高分辨率层序地层学 总被引：3，自引：0，他引：3
在准层序中进行层组一级地层单元的识别和对比是高分辨率层序地层学研究的主要难点.提出了一种综合应用井资料进行层组界面识别和对比的新方法.通过测井曲线形态特征、岩心观察、铸体薄片、X衍射、扫描电镜分析、FMI测井资料, 对工区内钙质夹层成因、泥岩电阻率差异、储层电阻率和海拔深度关系进行了研究.结果表明: 钙质夹层单层厚度在0.5~2m之间, 靠近风化壳和断层位置单层厚度大, 分布在水下分支河道底部和河口坝顶部; 低阻泥岩(4~5Ω·m)和高阻泥岩(> 10Ω·m) 分别来源于不同的沉积物源或者形成于不同的沉积相带; 储层电阻率随着海拔深度的增加而增加.因此, 钙质夹层可以作为层组界面识别和对比的标志, 利用泥岩电阻率差异可以确定层组的叠置关系, 判断储层连通性.据此, 建立了准噶尔盆地石南地区西山窑组含油层段等时地层格架, 确定了格架内储层的连通性及油水界面, 并且通过MDT测井资料进行了验证.在此等时地层格架内, 层组的发育顺序、叠置关系、空间展布形态、以及彼此之间的连通性都被定性、定量的表征出来. 相似文献
15.
Geophysical response of slackwater and sandy terrace deposits near Savanna, Northwestern Illinois 总被引：1，自引：1，他引：0
Low-permeability clayey and silty river terrace deposits are an important component in protecting underlying aquifers from contamination by agrochemicals and other contaminants. Such deposits also record deglaciation dynamics, meltwater drainage and local climatic variations. In this study, conducted over Mississippi River terraces near Savanna, Illinois, clayey slackwater terrace deposits and sandy terrace deposits are examined using resistivity soundings, ground-penetrating radar (GPR) profiles and direct-push conductivity logs. The clayey terrace deposits are characterized by low resistivity (10–35 ohm-m) and slow GPR wave velocity (0.07 m/ns), whereas non-clayey terrace deposits exhibit much higher resistivity (169–1,762 ohm-m) and faster GPR wave velocities (0.15 m/ns). Sandy and clayey terrace deposits may thus be differentiated and mapped on the basis of their geophysical response. Models based on resistivity soundings provide reasonably accurate estimates of the thickness of clayey slackwater deposits, but fail to reveal thin sands embedded in the clayey deposits. In some cases, the full thickness of the slackwater deposits was also not revealed. GPR profiles, however, imaged these embedded shallow sands and possibly imaged deeper sands below the base of the slackwater deposits, giving more accurate estimates of thickness. GPR also accurately resolved the thickness and character of sandy terrace deposits. Direct-push conductivity logs provide both accurate estimates of the thickness of clayey slackwater terrace deposits and a means of identifying thin embedded sands. In summary, resistivity soundings image these deposits at the lowest resolution with one-dimensional models, whereas GPR provides much higher resolution showing detailed layering within the upper several meters. Direct-push conductivity logs provide the highest resolution, but are invasive and only reveal stratigraphy at one location. 相似文献
16.
Bibi R. N. Gondwe David Ottowitz Robert Supper Klaus Motschka Gonzalo Merediz-Alonso Peter Bauer-Gottwein 《Hydrogeology Journal》2012,20(7):1407-1425
Geometry and connectivity of high-permeability zones determine groundwater flow in karst aquifers. Efficient management of karst aquifers requires regional mapping of preferential flow paths. Remote-sensing technology provides tools to efficiently map the subsurface at such scales. Multi-spectral remote sensing imagery, shuttle radar topography data and frequency-domain airborne electromagnetic (AEM) survey data were used to map karst-aquifer structure on the Yucatan Peninsula, Mexico. Anomalous AEM responses correlated with topographic features and anomalous spectral reflectance of the terrain. One known preferential flow path, the Holbox fracture zone, showed lower bulk electrical resistivity than its surroundings in the AEM surveys. Anomalous structures delineated inland were sealed above by a low-resistivity layer (resistivity: 1–5 Ωm, thickness: 5–6?m). This layer was interpreted as ejecta from the Chicxulub impact (Cretaceous/Paleogene boundary), based on similar resistivity signatures found in borehole logs. Due to limited sensitivity of the AEM survey, the subsurface configuration beneath the low-resistivity layer could not be unambiguously determined. AEM measurements combined with remote-sensing data analysis provide a potentially powerful multi-scale methodology for structural mapping in karst aquifers on the Yucatan Peninsula and beyond. 相似文献
17.
E.V. Onegova 《Russian Geology and Geophysics》2010,51(4):423-427
The article discusses the effect on the measured signals of a multicoil electromagnetic tool offset with respect to the borehole axis. The tool is a non-conductive cylindrical body with several coaxial coils. It is assumed that the borehole is vertical and the medium is axisymmetric with respect to the borehole axis.A number of computations based on the finite element method were carried out. Simulations took into account the tool body and finite sizes of coils. A wide range of transmitter-receiver spacings (0.18–1.0 m) was studied. The operating frequency was 1.75 MHz. Different drilling muds and values of the tool offset were examined. It was shown that, for highly conductive drilling muds, the type of dependence between apparent resistivity and eccentricity varies greatly with the array length. It was discovered that increasing the contrast between invaded zone resistivity and mud resistivity also increases the eccentricity effect. The eccentricity effect increases with the decrease in mud resistivity and decreases as the array length increases. Also analyzed was the effect of the tool offset on electromagnetic field pattern. 相似文献