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1.
在水介质中顺序添加分散粘土颗粒、油珠、导电骨架颗粒、层状泥质,并对每一种成分进行连续积分,建立了一种适用骨架导电及含有分散粘土和层状泥质的泥质砂岩通用电阻率模型.通过对该模型的影响因素分析,发现泥质分布形式对模型计算的含水饱和度有很大影响;对应两个不同粘土颗粒电阻率或骨架颗粒电阻率的地层电导率之差,几乎与总含水饱和度无关,而对应两个不同层状泥质电阻率的地层电导率之差,随总含水饱和度增大而增大;骨架胶结指数变化对地层电导率与总含水饱和度关系曲线的影响最大,而粘土胶结指数变化对地层电导率与总含水饱和度关系曲线的影响最小;饱和度指数对地层电导率与总含水饱和度关系曲线的影响随总含水饱和度的增大而减小.通过一组骨架导电的人造岩样的试验,表明当地层水电阻率.小于颗粒电阻率时,该模型可以用于不含粘土的骨架导电的岩石.通过两组分散泥质砂岩岩样实验测量数据和一组层状泥质砂岩测井资料及实际测井资料的计算,表明本文给出的电阻率模型既适用于分散泥质砂岩地层解释又适用于层状泥质砂岩地层解释,同时,还适用于含有分散粘土和层状泥质的混合泥质砂岩地层解释. 相似文献
2.
本文利用人工制作的不同含量分散泥质和层状泥质砂岩岩心样品,测量不同矿化度和不同含油饱和度的岩心电阻率,从实验角度研究了不同泥质分布形式和含量的岩心导电规律,结果表明,泥质分布形式或含量不同,则泥质砂岩导电规律不同.基于层状泥质与分散泥质砂岩的并联导电实验规律,以及分散粘土和地层水混合物的导电规律可用HB电阻率方程描述,建立了考虑泥质分布形式影响的泥质砂岩电阻率模型.通过1组不同泥质分布形式泥质砂岩人造岩心实验数据的测试,表明该模型可以描述分散泥质砂岩、层状泥质砂岩和混合泥质砂岩地层的导电规律.分散泥质,层状泥质,人造岩样,实验测量,并联导电,HB方程,电阻率模型 相似文献
3.
Shaly sands reservoir is one of the most distributive types of the oil(gas)-bearing reservoirs discovered in China, and low resistivity oil(gas)-bearing reservoirs are mostly shaly sands reservoirs. Therefore, shaly sands reservoir conductive model is the key to evaluate low resistivity oil(gas)-bearing reservoirs using logging information. Some defects were found when we studied the clay distribution type conductive model, dual-water conductive model, conductive rock matrix model, etc. Some models could not distinguish the conductive path and nature of microporosity water and clay water and some models did not consider the clay distribution type and the mount of clay volume. So, we utilize the merits,overcome the defects of the above models, and put forward a new shaly sands conductive model-dual water clay matrix conductive model (DWCMCM) in which dual water is the free water and the microporosity water in shaly sands and the clay matrix(wet clay) is the clay grain containing water. DWCMCM is presented here, the advantages of which can tell the nature and conductive path from different water (microporosity water and freewater), in consid-eration of the clay distribution type and the mount of clay volume in shaly sands. So, the results of logging interpretation in the oil(gas)-bearing reservoirs in the north of Tarim Basin area, China with DWCMCM are better than those interpreted by the above models. 相似文献
4.
The conductance of pyrite-bearing laminated and dispersed shaly sands is not well understood and resistivity models for pyrite-bearing shaly sands are nonexistent. Thus, we first synthesize clean pyrite-matrix samples, and quartz-matrix samples with variable laminated shale, dispersed shale, and pyrite content and then perform petrophysics experiments to assess the effect of pyrite content on the conductivity of pyrite-bearing shaly sands. Second, based on the differences in conductivity and conduction pathways and geometries because of the variable composition of the pyrite-bearing laminated and dispersed shaly sands, we divide the shaly sands into their components, i.e., laminated shale, quartz grains, pyrite grains, hydrocarbon, dispersed shale, microscopic capillary water, and mobile water. A generalized resistivity model is proposed to describe the conductivity of pyrite-bearing laminated and dispersed shaly sands, based on the combined conductivity differential equation and generalized Archie equation. In the generalized resistivity model, the conductivity differential equation is used to describe the conductivity of dispersed inclusions in a host, whereas the generalized Archie equation is used to describe the conductivity of two conducting phases. Moreover, parallel conductance theory is used to describe the conductivity of dispersed shaly sands and laminated shale. Theoretical analysis suggests that the proposed model satisfies the physical constraints and the model and experimental results agree. The resistivity and resistivity index of shaly sands decrease with increasing conductivity and pyrite. Finally, the accuracy of the resistivity model is assessed based on experimental data from 46 synthetic core samples with different oil saturation. The model can describe the conductivity of clean pyrite-matrix samples, and quartz-matrix samples with different volumes of laminated shale, dispersed shale, and pyrite. An accurate saturation model of pyrite-bearing laminated and dispersed shaly sands is thus obtained and the log data interpretation in complex shaly sands can improve with the proposed model. 相似文献
5.
Heping Pan Jiaying Wang Zhengjun Fan Yong Ma Jianhua Liu Mingqiang Li 《中国科学D辑(英文版)》2001,44(4):346-355
Shaly sands reservoir is one of the most distributive types of the oil(gas)-bearing reservoirs discovered in China, and low resistivity oil(gas)-bearing reservoirs are mostly shaly sands reservoirs. Therefore, shaly sands reservoir conductive model is the key to evaluate low resistivity oil(gas)-bearing reservoirs using logging information. Some defects were found when we studied the clay distribution type conductive model, dual-water conductive model, conductive rock matrix model, etc. Some models could not distinguish the conductive path and nature of microporosity water and clay water and some models did not consider the clay distribution type and the mount of clay volume. So, we utilize the merits,overcome the defects of the above models, and put forward a new shaly sands conductive model—dual water clay matrix conductive model (DWCMCM) in which dual water is the free water and the microporosity water in shaly sands and the clay matrix(wet clay) is the clay grain containing water. DWCMCM is presented here, the advantages of which can tell the nature and conductive path from different water (microporosity water and free-water), in consideration of the clay distribution type and the mount of clay volume in shaly sands. So, the results of logging interpretation in the oil(gas)-bearing reservoirs in the north of Tarim Basin area, China with DWCMCM are better than those interpreted by the above models. 相似文献
6.
泥页岩储层储集空间以纳米/微米级的微孔隙和微裂缝为主,结构复杂,加之干酪根和黏土矿物含量较高,并含有一定量的黄铁矿等导电矿物,造成储层导电机理异于常规储层,岩电实验I-S_w曲线呈现非线性特征,阿尔奇公式等传统评价模型适用性较差.针对上述问题,根据实际岩心实验资料,结合随机算法建立三维逾渗模型并通过数值模拟和超松弛迭代法进行求解,分析泥页岩储层非阿尔奇性产生原因以及泥页岩储层电性的影响因素及规律.模拟结果显示,岩石孔隙拓扑结构和形状尺寸、矿物组成以及地层水电阻率等因素均对泥页岩储层电阻率产生不同程度的影响,通过改变上述因素的设定值,可以建立储层电阻率与各因素的单相关关系,并据此建立修正模型,实现储层含水饱和度的计算.该模型在四川某页岩气产区取得了较好的效果,具有良好的应用前景,为利用逾渗模型模拟方法解决油田勘探开发中的复杂问题提供了新思路. 相似文献
7.
研究了淡水环境下富含粘土矿物、细颗粒砂岩低电阻率油气层. 分析了粘土的附加导电性,认为粘土质量百分数高且富含伊利石和蒙脱石的地层中,若地层水质量浓度小于15g/L等效NaCl盐溶液时,粘土的附加导电性是造成油气层电阻率低的首要原因. 同时分析了细颗粒、粘土质量百分数不高的储层,高的毛细管压力使束缚水饱和度很高,同样能形成低电阻率油气层. 储层中粘土质量百分数的多少对储层岩石电性特征(I-Sw曲线形态)有重要影响,可用于指导测井资料解释模型的选择. 相似文献
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低渗透岩性油气藏发育的黏土膜吸附原油造成了储层亲油,电阻率异常高,高阻油水层、水层的存在给储层流体性质识别带来了很大挑战.为了明确不同润湿性储层的电阻率响应特征以及微观导电机理,本文选取了鄂尔多斯盆地西部三叠系延长组长8段的岩心,模拟了油驱水、老化和水驱油过程,并测量了岩心薄片洗油后的接触角.实验结果表明,洗油后异常高阻岩心已表现为不完全亲水,然而,其测量的胶结指数m与正常电阻率岩心相差很小.油驱水至束缚水时,正常电阻率岩心的电阻增大率I_r与含水饱和度Sw的关系在双对数坐标下基本表现为直线的关系,而异常高阻岩心则表现为明显的凸曲线特征.且老化过程前后,异常高阻岩心的电阻率基本不变.结合对异常高阻岩心不同状态下的核磁共振T_2谱的分析,表明在油驱水过程中,岩石的润湿性已经向亲油方向发生转变,老化过程对润湿性的改变影响很小.水驱油至残余油时,异常高阻岩心的I_r-S_w曲线表现为近似直线特征,反映出水驱油过程中岩石的导电结构并未发生改变.基于实验结果的分析与讨论,明确了一种适用于低渗透复杂润湿性储层的成藏模式及其导电机理,说明了高阻水层主要是亲油润湿性条件下的连续导电路径遭到破坏造成的. 相似文献
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油层注入聚合物溶液后,电阻率测井响应发生与水驱不同的变化特征,严重影响水淹层测井评价的效果。本文首先分析了聚合物溶液的导电性质,其次按照聚合物驱油层不同施工流程开展岩电实验研究,分析不同驱替阶段的岩石电阻率的变化特征。并对比分析聚合物驱与水驱油层电阻率测井响应的差异。结果表明,不同聚合物驱替饱含油岩心过程,岩心电阻率随饱和度变化呈现"w"型或"S"型和单调下降的形态;清水聚合物驱油层电阻率测井响应呈现弱、未水淹的特征;污水聚合物驱油层电阻率测井响应呈现与污水水驱相似的变化特征。 相似文献
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液相渗透率描述了岩石的渗流特性,是评价储层与预测油气产能的重要参数.液相渗透率是指盐水溶液在岩石孔隙中流动且与岩石孔隙表面黏土矿物发生物理化学作用时所测得的渗透率;液相渗透率的实验测量条件更加接近实际地层泥质砂岩的条件,使得液相渗透率更能反映地层条件下泥质砂岩的渗流特性;然而,现有的液相渗透率评价模型较少,且模型未能揭示液相渗透率与溶液矿化度之间的关系.基于此,开展了液相渗透模型推导与计算方法研究;文中首先将岩石等效为毛管束模型,推导建立了液相渗透率与比表面、喉道曲折度、总孔隙度、黏土束缚水孔隙度等参数之间的关系;其次,根据岩石物理体积模型,推导建立了黏土束缚水孔隙度与阳离子交换容量、溶液矿化度等参数的关系;最终,将黏土束缚水孔隙度引入液相渗透率计算公式,建立了基于总孔隙度、阳离子交换容量、溶液矿化度、比表面、喉道曲折度等参数的液相渗透率理论计算模型.液相渗透率计算模型与两组实验数据均表明,液相渗透率随阳离子交换容量的增大而降低,随溶液矿化度的增大而增大.然而,液相渗透率理论计算模型的实际应用中喉道曲折度、比表面等参数求取困难,直接利用理论模型计算液相渗透率受到限制.在分析液相渗透率与孔隙渗透率模型的基础上,建立了液相渗透率与空气渗透率之间的转换模型,形成了利用转化模型计算液相渗透率的新方法.为进一步验证液相渗透率与空气渗透率转化模型的准确性,基于两组实验数据,利用转换模型计算了液相渗透率;液相渗透率计算结果与岩心测量液相渗透率实验结果对比显示,液相渗透率计算结果与实际岩心测量结果吻合较好,文中建立的液相渗透率与空气渗透率转化模型合理可靠. 相似文献
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针对鄂尔多斯盆地陕北斜坡长6特低渗透储层受聚合物泥浆伤害,微电极电阻率曲线在渗透层上的正幅度差异不明显,直观指示油气层和水层的深、中,浅探测电阻率在常规储层的有序排列基本消失.通过注聚合物泥浆驱替前后岩石电阻率与孔隙度及含水饱和度实验关系分析,驱替后岩样电阻率显著增大,岩样电阻率随含水饱和度增大而减小的基本规律不复存在.归纳其岩性系数a、电阻率系数b比驱替前大得多,饱和度指数n由正变负,反映出注聚合物泥浆驱替破坏了储层孔隙结构及其基本特征,测井中造成了范围较小的高侵和特高侵地层电阻率带.从而提出在较为致密的低渗砂、致密砂聚合物泥浆伤害储层中,利用微电极负差异及其电阻率曲线不规则增高变化划分特低渗透油层有效厚度,并以实例阐明了利用岩电实验参数变化评价特低渗透储层的方法. 相似文献
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为了进一步认识泥质对岩石宏观电性的影响规律，本文利用非规整三维逾渗网络模型，通过数值模拟研究了不同矿化度下泥质对岩石电性影响的规律. 模拟结果表明：在中低矿化度下，泥质对岩石导电整体上呈现减阻作用，随着泥质含量的增加，电阻率降低的速度减慢；中等矿化度下泥质的减阻效果明显弱于低矿化度下的减阻效果；在高矿化度下泥质对岩石导电整体上呈现增阻作用. 在高矿化度、高含水饱和度下泥质对岩石电性的影响较小. 泥质起减阻、增阻作用的具体矿化度范围取决于储层的孔隙度、连通性以及地层温度等特性. 相似文献
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George F. Risk T. Grant Caldwell Hugh M. Bibby 《Journal of Volcanology and Geothermal Research》2003,127(1-2):33-54
Experimental measurements in the Ngatamariki geothermal field, North Island, New Zealand were made to test the applicability of the time domain electromagnetic method for detailed investigation of the resistivity structure within a geothermal field. Low-frequency square wave signals were transmitted through three grounded bipole current sources sited about 8 km from the measurement lines. Despite high levels of electrical noise, transient electric field vectors could be determined reliably for times between 0.02 and 3.3 s after each step in the source current. Instantaneous apparent resistivity tensors were then calculated. Apparent resistivity pseudosections along the two measurement lines show smooth variations of resistivity from site to site. Over most of the field the images consistently show a three-layer resistivity structure with a conductive middle layer (3–10 Ωm) representing the conductive upper part of the thermal reservoir. A deep-seated region of low resistivity in the northwest of the field may indicate a conductive structure at about 1 km associated with a deeper diorite intrusion. Measurements sited closer than about 100 m to drillholes appear to have been disturbed by metallic casing in the holes. A change in resistivity structure in the east of the field may indicate a major geological or hydrothermal boundary. 相似文献
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碳酸盐岩储层孔隙类型多样,各种孔隙的尺寸变化范围可以跨越几个数量级,孔隙结构非常复杂,这种复杂孔隙结构和不均匀分布的多元孔隙空间使得储层电性呈现明显非阿尔奇特性.为了了解影响电阻率变化的控制因素,本次研究选取中三叠世雷口坡组的8块全直径碳酸盐岩岩样,开展了核磁共振、岩电实验、孔渗实验、压汞实验及薄片等实验,并利用数字图像分析法定量分析了孔隙结构特征.研究结果表明：①孔隙度是影响电阻率高低的重要因素,但并非唯一因素,除孔隙度以外,孔隙尺寸和数量、孔隙网络复杂程度远比吼道大小对电阻率的影响大;②在孔隙度一定的条件下,胶结指数m随储层中孤立大孔隙占比的增多而增大,当孔隙度增大到一定程度后,胶结指数m又随大孔隙占比的增多而减小,微裂缝起重要沟通作用;③在给定孔隙度时,以简单大孔隙为主的岩样表现为胶结指数m值较大,而以复杂孔隙网络、细小孔隙为主的岩样表现为胶结指数m值较小,具分散、孤立大孔隙的岩样,胶结指数m值最高;④依据孔隙几何参数与电阻率和胶结指数之间的关系,可以利用测井资料间接判别储层类型,从而提高储层有效性和含水饱和度评价精度. 相似文献
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The properties of rock resitivity were studied under pressure, particularly with “stress reversal”, a procedure in which the
pressure applied was increased and decreased.
It was observed that, 1) With pressure increasing, the main feature of resistivity change was increase-steady-decrease for
high-saturation rock samples (saturation 70–100%). But the main feature for low-saturation samples was different. 2) In 10
out of 11 cases of “stress reversal” for high-saturation samples the resistivity droped (about 2%). Such drop could explain
the anomalies in geoelectricity terms, which are commonly observed before earthquakes in China. 3) It was also observed shortly
before rock failure that, a) the resistivity drops more dramatically (about 20%) during “stress reversal” period, which is
much more than ordinary drops. b) these drops occurred not only during stress decrease but also during stress increase. c)
Resistivity exhibits anisotropy: the resistivity along different directions may differ by 10%. These three features may indicate
that the rock is nearing failure, while ordinary resistivity drops are only connected with “stress reversal” and may not mean
the imminence of rock failure. 4) Resistivity increase was observed during the “stress reversal” period for low-saturation
rock samples.
The results mentioned above were explained with the effect of water flowing in and out of the cracks of rock. The temporary
factors which yield a reduction of the maximum main stress, may enhence the possibility of earthquake occurrence. 相似文献
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针对泥质砂岩黏土附加导电还没有综合定量评价指标的现状，从Archie公式和Waxman-Smits方程计算的含水饱和度的相对误差出发定义了黏土附加导电强度指数η，并考察了地层水电导率Cw、阳离子交换容量Qv、含水饱和度Sw、饱和度指数n对η的影响，给出了黏土附加导电强度判别方法和图版，通过低阻油气层的工程应用实例探讨了η在饱和度方程选取中的应用.结果表明，η随Cw、Sw、n值的增大而以近似乘幂规律减小，随Qv的增大而近似线性增大；Cw与Qv对η的影响最大，n与Sw次之；无法由单一因素判断黏土附加导电性强弱，必须综合考虑Qv、Cw、Sw、n的影响；对于低阻油气层，可利用该指数按照"三步法"及判别图版定量判断低阻成因并为饱和度模型的选取提供技术依据. 相似文献
20.
讨论了强地震、孕震晚期阶段、震源区及附近介质的物理变化过程，证明了视电阻率变化最显著的方向与最大加载方向之间的正交关系，建立了真、视电阻率各向异性变化与裂隙率ν、骨架电阻率ρo、饱水裂隙电阻率ρf的本构关系，解释了视电阻率各向异性变化的原因.研究认为：在强地震孕震晚期阶段，在震源区及附近地壳近地表的较深部，介质微裂隙发育，其走向沿最大主压应力方位优势取向，低阻水充填微裂隙，导电通道连通，引起最大主压应力方向真电阻率变化最显著的真各向异性变化，从而产生垂直主压应力方向视电阻率变化最显著的视各向异性变化，低阻水在其物理过程中起了显著作用. 相似文献