共查询到19条相似文献，搜索用时 625 毫秒
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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
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《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
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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
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低阻油层的电测井资料反演与动态侵入模拟 总被引：1，自引：0，他引：1
高矿化度钻井液侵入是造成油层低电阻的重要因素之一,泥浆滤液侵入越深,对测井结果影响越大,甚至造成解释错误或油层漏失.采用非线性最小二乘原理进行电测井反演预处理,并将其同以多相流渗流、对流扩散理论为基础的电测井动态模拟相结合,能更加真实地反映动态侵入特点,获取原状地层真电阻率和流体饱和度,从而有效地改善低电阻率油气层电测井资料的有效性,为低电阻率油层的识别和评价提供可靠的依据. 相似文献
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油气藏上方存在自然电位异常,经典理论认为这是由于氧化还原电池效应所产生的.但这种观点无法解释油气藏上方自然电位异常空间变化大,甚至还出现明显的正异常现象.模拟油气微渗漏气泡上升迁移的实验表明,由于气水界面偶电层具有明显的负ζ电位,不同数量气泡在不同盐度水溶液中上升迁移时均起着一种天然的负电荷流的作用,因此可产生一定的自然电场.在此基础上,建立了油气微渗漏气体运移生电模型.该模型为自然电位资料预测油气藏的埋藏深度提供了定量解释依据.初步研究表明,自然电场的性质和异常强度与地面测量资料有较好的一致性. 相似文献
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声波时差测井资料识别层序地层单元界面的方法、原理及实例 总被引：11，自引：2，他引：11
结合济阳坳陷古近系层序地层研究,在地震、岩芯、录井等资料综合分析基础上,探讨了运用声波时差测井识别层序地层单元界面的方法和原理。在正常埋藏压实条件下,泥页岩的声波时差对数与其深度的关系曲线为一条直线(回归线),由于沉积作用形成的不整合造成地层缺失、风化层和致密的湖侵泥岩层形成等,将使不整合面(层序界面)上下的声波时差对数与深度的回归线出现错开、斜率不同、异常值等异常响应。生油岩密集段(CS段)在湖盆洼陷带对应于泥岩、页岩沉积,有机质含量高,声波时差值也高,并且同一层序内在最大湖泛面位置声波时差值达到最大,向上、向下均逐渐减小,在层序界面附近达到最小。 相似文献
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双侧向测井曲线形状的影响因素研究 总被引：2，自引：0，他引：2
为研究井眼、层厚和侵入带对双侧向测井曲线形状的影响,利用正演模拟技术分别对各种常见情况计算了双侧向曲线。结果显示,井径增大使曲线变化趋缓,且幅度降低;泥浆电阻率与地层电阻率反差的增加则使曲线棱角更加分明;层厚在1m以下时高侵层无双尖峰现象,2m以上厚层曲线形态变化不大,低侵层厚度〉4m时,曲线在地层中部开始出现平顶;侵入带厚度较小时,曲线的侵入特征更明显,厚度大时趋于无侵入高阻层的形态;侵入带与地层和围岩的电阻率对比决定曲线的形状和幅度。 相似文献
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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
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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
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水平井和大斜度井中阵列侧向测井响应数值模拟 总被引：1，自引：0，他引：1
针对水平井和大斜度井中阵列侧向电极系的工作原理,利用多电场叠加方式进行电场合成,采用三维有限元方法模拟仿真各个分电场的场分布,进而利用电场线性叠加原理得到阵列侧向测井响应。在基于计算机仿真的基础上,得到阵列侧向五条测井曲线的径向探测深度,阵列侧向径向探测深度要小于深侧向探测深度。考察了三维地层模型下井斜和侵入深度变化对阵列侧向测井响应的影响,分析了水平井和大斜度井中阵列侧向测井响应特征。模拟结果表明,在井斜小于15°时,阵列侧向测井响应受井斜影响小,可以不进行井斜校正;井斜超过60°的大斜度井以及水平井中,阵列侧向测井响应视地层厚度逐渐增大,测井响应值与直井条件下响应值差别较大,必须进行井斜校正。 相似文献
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We re-processed the seismic reflection survey data of the Kakkonda geothermal field. The pre-stack migration delineates a strong and continuous reflector between 1800- and 2800-m depth, below which formations are not reflective. Earthquake data exhibit seismicity in the upper crust. The lower boundary of seismogenic layer is interpreted as the brittle–ductile transition. The thermal structure is thought to be the major factor controlling its depth. We compared the strong reflector with the thermal and rheological structure from drillholes. The depth of the reflector corresponds to the top of the highly–very highly fractured zone observed from formation microscanner imagery (FMI) logging in the Miocene formations. The density of fracture in the Kakkonda granite is very low, suggesting that granite corresponds to the nonreflective zone. The temperature–depth profile of well WD-1a shows that the temperature at the highly–very highly fractured zone is about 350 °C. This corresponds to a hydrothermal convection zone filled with two-phase geothermal fluid. The cut-off depth of seismicity that indicates the brittle–ductile transition lies at the isotherm of 300–350 °C near the reflector. We conclude that the strong seismic reflector is a strong contrast in acoustic impedance at the top of the fractured layer. The fractured layer could be a decoupling plane caused by different tectonic behaviors between the upper brittle and the lower ductile layers or a dehydration front by thermal diffusion. The similarity between the strong reflector and K-horizon, the strong reflector, found in southern Tuscany, Italy suggests that the P-wave reflector at the top of highly fractured zone at the brittle–ductile transition be common in areas with magmatic activity. 相似文献
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L. L. Kitchatinov 《Astronomy Reports》2006,50(11):944-950
The tachocline is a thin layer providing the transition from differential to uniform rotation in the upper region of the solar radiative zone, which can be explained as an effect of the magnetic field if the magnetic field lines are closed inside the radiative zone. It is shown that the confined field structure that is necessary for the tachocline formation can arise due to the penetration of meridional flow from the convective envelope to the radiative zone. The time for the distortion of the magnetic field by the penetrating flow is short compared to the time for diffusion to the penetration depth. The most long-lived mode of the poloidal field has a confined geometry, and the Ohmic lifetime of this mode exceeds the age of the Sun. The calculated distribution of the angular velocity in the radiative zone taking into account such a field shows a thin tachocline. 相似文献
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采煤塌陷引起的地裂缝不仅造成地质灾害,还会影响矿区植被的生长发育,破坏矿区生态系统。为深入探讨采煤塌陷裂缝对沙蒿吸水来源的定量影响,在神东矿区活鸡兔井田22312工作面选取了受采煤塌陷裂缝影响程度不同的3个试验区进行同位素标记水模拟降水试验。3个试验区根据沙蒿与裂缝的距离不同划分,其采煤塌陷情况分别为未开采区(试验样地内沙蒿距离裂缝大于50 m)、受采煤塌陷影响但无明显裂缝区(简称无明显裂缝区,试验样地内沙蒿距离裂缝大于5 m)以及裂缝区(试验样地内分布有宽度15 cm左右的裂缝通过,且距离沙蒿0~20 cm)。本次试验选择6株沙蒿作为研究对象,划分6个土壤剖面,采用液态水同位素分析仪LGR和Isoprime 100同位素比值质谱仪IRMS分别计算不同土层土壤水和植物样本木质部水的δ18O和δ2H同位素含量,并利用R脚本的MixSIAR贝叶斯混合模型量化降水后不同土层对沙蒿吸水的贡献,探讨土壤水分补给机制和植物水分来源。结果表明:(1) 裂缝区的优先流比例为18.2%;(2) 在未开采区,沙蒿吸收的59.7%的水分来自10~20 cm的土层;(3) 在无裂缝区,沙蒿主要从40~60 cm土层(46.6%)和0~10 cm土层(39.4%)吸水;(4) 在裂缝区,沙蒿吸收的85.9%的水分主要来自40~60 cm的土层。研究结果对揭示采煤塌陷裂缝区土壤水补给机制以及沙蒿吸水模式具有重要意义。 相似文献
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冻结滞水形成机制的探讨 总被引：11，自引：4，他引：11
资料表明，冻结滞水形成机制是在冬季的冻结作用下，包气滞冻土层内产生氢键吸附能，饱和水汽压差和气管薄膜等机制构成冻结势。它具用奶强的吸附能凝聚水分，全副钨气带水和潜水液态，汽态向冻结层迁移富集；形成季节性固态地下水。在冻结期间包气带水盐具有明显倒置分带性：冻结滞水带；过渡水分带；支持毛管水汽化输水带。 相似文献
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可控源音频大地电磁(CSAMT)是探测含煤地层富水区及采空区的重要地球物理方法,但其探测深度误差比较大,采用电性标志层进行深度校正,达到精确解释地层的目的。首先,提出基于电场单分量视电阻率计算方法,只需通过平移即可获得全区视电阻率,无需迭代,简单快速。接着,分析视电阻率微分极值与电性标志层的关系,通过测井电阻率曲线识别出电性标志层,然后通过比值计算深度校正系数,在全区进行插值得到任意测点的校正深度。对新元煤矿31004工作面R280测线数据进行深度校正处理,结果表明:校正后的深度和实际地层基本吻合。最后,通过已知充水采空区边界、淋水点以及钻孔揭示的结果进行对比验证,达到了预期效果。该方法为CSAMT在含煤地层进行精细化数据处理和解释提供了新的思路。 相似文献