CN115898368A - A Method for Extracting Anisotropic Resistivity of Horizontal Well Shale Oil Reservoir - Google Patents

A Method for Extracting Anisotropic Resistivity of Horizontal Well Shale Oil Reservoir Download PDF

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CN115898368A
CN115898368A CN202211407726.8A CN202211407726A CN115898368A CN 115898368 A CN115898368 A CN 115898368A CN 202211407726 A CN202211407726 A CN 202211407726A CN 115898368 A CN115898368 A CN 115898368A
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赵伟娜
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Qingdao University of Technology
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Abstract

本发明公开了一种水平井页岩油储层各向异性电阻率提取方法,包括:获取邻井信息,以及水平井阵列感应测井N个子阵列及合成的视电阻率曲线;基于短源距子阵列曲线以及实测GR曲线,划分水平井地层界面;建立解释模型,构建层状各向同性处理模型M1和均质各向异性处理模型M2;反演第i个子阵列曲线,获得地层电阻率剖面,并将其作为下一长源距子阵列的初值;依次反演各子阵列视电阻率曲线,获得相应的地层电阻率剖面;对第j个地层,采用模型M2,反演当前层的各向异性电阻率Rhj和Rvj;循环,得到各个地层的各向异性电阻率。该方法准确提取页岩油储层各向异性电阻率信息,有效消除井斜、围岩和各向异性对测井响应的影响,保证储层含油饱和度计算的精度。

Figure 202211407726

The invention discloses a method for extracting the anisotropic resistivity of a horizontal well shale oil reservoir, comprising: obtaining adjacent well information, and horizontal well array induction logging N sub-arrays and synthesized apparent resistivity curves; Sub-array curves and measured GR curves are used to divide the formation interface of horizontal wells; interpretation models are established to construct layered isotropic processing model M 1 and homogeneous anisotropic processing model M 2 ; the ith sub-array curve is inverted to obtain formation resistance and take it as the initial value of the next long source spacing sub-array; invert the apparent resistivity curves of each sub-array in turn to obtain the corresponding formation resistivity profile; for the jth formation, use the model M 2 to invert The anisotropic resistivity R hj and R vj of the current layer; cycle to obtain the anisotropic resistivity of each formation. This method accurately extracts the anisotropic resistivity information of shale oil reservoirs, effectively eliminates the influence of well deviation, surrounding rock and anisotropy on the logging response, and ensures the accuracy of reservoir oil saturation calculation.

Figure 202211407726

Description

一种水平井页岩油储层各向异性电阻率提取方法A Method for Extracting Anisotropic Resistivity of Horizontal Well Shale Oil Reservoir

技术领域technical field

本发明涉及石油勘探开发技术领域,属于电测井方法范畴,尤其涉及一种水平井页岩油储层各向异性电阻率提取方法。The invention relates to the technical field of petroleum exploration and development, belongs to the category of electrical logging methods, and in particular relates to a method for extracting the anisotropic resistivity of a horizontal well shale oil reservoir.

背景技术Background technique

阵列感应测井广泛应用于油气资源勘探中,对于页岩油储层具有显著的特征,其侵入异常小且广泛应用于油基泥浆。而斜井和水平井中曲线的分离导致饱和度参数不准确,在层厚影响下合成曲线无法反映地层真实信息。但是,水平井中阵列感应测井响应的模拟通常采用三维处理方法,计算精度低、速度慢,同时在水平井中受仪器倾斜、泥浆滤液侵入等多种因素影响严重,不能准确反映真实地层情况。目前,对于水平井电阻率的精确提取方法较少,亟需研发新的水平井各向异性电阻率提取方法,用于有效测量水平井中页岩油储层各向异性电阻率信息。Array induction logging is widely used in the exploration of oil and gas resources, and has remarkable characteristics for shale oil reservoirs. Its invasion is abnormally small and it is widely used in oil-based mud. However, the separation of curves in deviated wells and horizontal wells leads to inaccurate saturation parameters, and the synthetic curves cannot reflect the real information of formations under the influence of layer thickness. However, the simulation of array induction logging response in horizontal wells usually adopts three-dimensional processing method, which has low calculation accuracy and slow speed. At the same time, in horizontal wells, it is seriously affected by various factors such as instrument tilt and mud filtrate invasion, and cannot accurately reflect the real formation conditions. At present, there are few accurate extraction methods for the resistivity of horizontal wells, and it is urgent to develop a new method for extracting the anisotropic resistivity of horizontal wells to effectively measure the anisotropic resistivity information of shale oil reservoirs in horizontal wells.

发明内容Contents of the invention

为解决上述技术问题,本发明公开了一种水平井页岩油储层各向异性电阻率提取方法,该方法基于阵列感应测井原始信号,以期为页岩油储层评价提供准确地层信息。In order to solve the above technical problems, the present invention discloses a method for extracting the anisotropic resistivity of horizontal well shale oil reservoirs. The method is based on the original signal of array induction logging, in order to provide accurate formation information for shale oil reservoir evaluation.

为实现上述目的,本发明采用下述技术方案:To achieve the above object, the present invention adopts the following technical solutions:

一种水平井页岩油储层各向异性电阻率提取方法,包括如下步骤:A method for extracting the anisotropic resistivity of a horizontal well shale oil reservoir, comprising the steps of:

s1.获取邻井地层层厚、地层水平电阻率、自然GR曲线信息,以及实测水平井阵列感应测井N个子阵列及合成的视电阻率曲线,其中,水平井阵列感应测井子阵列包括短源距子阵列和长源距子阵列;s1. Obtain the formation thickness, formation horizontal resistivity, and natural GR curve information of adjacent wells, as well as the measured horizontal well array induction logging N subarrays and the synthesized apparent resistivity curves, wherein the horizontal well array induction logging subarray includes short source-spacing subarrays and long-source-spacing subarrays;

s2.基于短源距子阵列曲线以及实测水平井GR曲线,划分水平井地层界面;s2. Based on the short source distance sub-array curve and the measured horizontal well GR curve, divide the formation boundary of the horizontal well;

s3.建立解释模型,构建层状各向同性处理模型M1和均质各向异性处理模型M2s3. Establish an interpretation model, construct a layered isotropic processing model M 1 and a homogeneous anisotropic processing model M 2 ;

s4.反演第i个子阵列曲线,获得地层电阻率剖面Rtsi,并将该结果作为下一长源距子阵列的初值;s4. Invert the i-th subarray curve to obtain the formation resistivity profile Rts i , and use this result as the initial value of the next long source distance subarray;

s5.依次反演各子阵列视电阻率曲线,分别获得相应的地层电阻率剖面Rtsi,i=1,…,N;s5. Inverting the apparent resistivity curves of each sub-array in turn to obtain the corresponding formation resistivity profiles Rts i , i=1,...,N;

s6.对层状各向同性处理模型M1中第j个地层,结合步骤s5的反演结果,采用均质各向异性处理模型M2,反演当前层的各向异性电阻率Rhj和Rvjs6. For the jth formation in the layered isotropic processing model M 1 , combined with the inversion results in step s5, use the homogeneous anisotropic processing model M 2 to invert the anisotropic resistivity R hj and R vj ;

s7.依次循环步骤s6,处理层状各向同性处理模型M1中每一层,进而得到各个地层的各向异性电阻率。s7. Step s6 is repeated sequentially to process each layer in the layered isotropic processing model M1 , and then obtain the anisotropic resistivity of each formation.

可选地,步骤s3包括如下步骤:Optionally, step s3 includes the following steps:

s3.1.针对页岩油储层电性特征和钻井环境,考虑井眼、地层褶皱、层厚和井斜影响,建立实际地层模型;s3.1. Based on the electrical characteristics of shale oil reservoirs and the drilling environment, consider the effects of wellbore, formation folds, layer thickness and well deviation, and establish an actual formation model;

s3.2.忽略地层褶皱影响,对步骤s1中N个子阵列信号进行井眼校正后,建立相应的解释模型;s3.2. Neglecting the influence of formation folds, after performing borehole correction on the N subarray signals in step s1, a corresponding interpretation model is established;

s3.3.分别考虑层厚和各向异性影响,将地层等效为有层厚影响无各向异性影响地层和有各向异性无层厚影响地层,进而依次构建层状各向同性处理模型M1和均质各向异性处理模型M2s3.3. Considering the influence of layer thickness and anisotropy respectively, the stratum is equivalent to the stratum with thickness influence and no anisotropy influence and the stratum with anisotropy and no thickness influence, and then sequentially builds the layered isotropic processing model M 1 and homogeneous anisotropic processing model M 2 ;

s3.4.层状各向同性处理模型M1包括参数Rtsi、θ和Hj,其中,Rtsi为等效各向同性电阻率,Hj为地层厚度,θ为井斜,i代表第i个子阵列,j代表第j个地层,层状各向同性处理模型M1用于消除层厚影响;s3.4. Layered isotropic processing model M 1 includes parameters Rts i , θ and H j , where Rts i is equivalent isotropic resistivity, H j is formation thickness, θ is well deviation, and i represents the first i sub-arrays, j represents the jth formation, and the layered isotropic processing model M1 is used to eliminate the influence of layer thickness;

s3.5.均质各向异性处理模型M2包括参数Rhj、θ和Rvj,其中,Rhj为水平电阻率,Rvj为垂向电阻率,θ为井斜,j代表第j个地层,均质各向异性处理模型M2用于获得各向异性信息。s3.5. The homogeneous anisotropy processing model M 2 includes parameters R hj , θ and R vj , where R hj is the horizontal resistivity, R vj is the vertical resistivity, θ is the well deviation, and j represents the jth Stratigraphic, homogeneous anisotropy processing model M2 is used to obtain anisotropy information.

可选地,步骤s4包括如下步骤:Optionally, step s4 includes the following steps:

s4.1.利用邻井参考电阻率、水平井实测子阵列曲线及合成曲线,提供反演初值;s4.1. Use the reference resistivity of adjacent wells, the measured sub-array curves and synthetic curves of horizontal wells to provide initial values for inversion;

s4.2.对第一个子阵列曲线,结合步骤s4.1提供的反演初值与步骤s3中构建的层状各向同性处理模型M1,反演获得地层电阻率剖面Rtsi,并将该结果作为下一个长源距子阵列的初值;s4.2. For the first sub-array curve, combine the inversion initial value provided in step s4.1 with the layered isotropic processing model M 1 constructed in step s3, invert to obtain the formation resistivity profile Rts i , and Use the result as the initial value of the next long source distance subarray;

s4.3.对第i个子阵列曲线,将前一子阵列反演得到的地层电阻率剖面Rtsi-1作为反演初值,反演获得地层电阻率剖面Rtsi,并将该结果作为下一长源距子阵列的初值。s4.3. For the ith sub-array curve, use the formation resistivity profile Rts i-1 obtained from the inversion of the previous sub-array as the inversion initial value, invert to obtain the formation resistivity profile Rts i , and use this result as the following The initial value of a long-distance subarray.

可选地,步骤s6包括如下步骤:Optionally, step s6 includes the following steps:

s6.1.步骤s3建立的均质各向异性处理模型M2,包括参数Rh和Rv,其中,Rh为水平电阻率,Rv为垂向电阻率,该模型忽略层厚影响;s6.1. The homogeneous anisotropy processing model M 2 established in step s3 includes parameters R h and R v , wherein R h is the horizontal resistivity, R v is the vertical resistivity, and this model ignores the influence of layer thickness;

s6.2.对层状各向同性处理模型M1中第j个地层,将步骤s5得到的当前层的N个电阻率剖面作为反演输入信息,结合步骤s3中构建的均质各向异性处理模型M2,对步骤s5的解释结果进行反演,得到当前层的各向异性电阻率Rhj和Rvjs6.2. For the jth formation in the layered isotropic processing model M1 , use the N resistivity profiles of the current layer obtained in step s5 as inversion input information, combined with the homogeneous anisotropy constructed in step s3 Process the model M 2 , invert the interpretation result of step s5, and obtain the anisotropic resistivity R hj and R vj of the current layer;

s6.3.将层状各向同性处理模型M1中的所有层进行逐层反演,重复上述过程,从而获得各个地层的各向异性电阻率。s6.3. Perform layer-by-layer inversion of all layers in the layered isotropic processing model M1 , and repeat the above process to obtain the anisotropic resistivity of each formation.

本发明的有益效果是,本发明给出了一种基于阵列感应测井原始信号的水平井页岩油储层各向异性电阻率提取方法,充分利用邻井信息,确定层界面位置,并为后续处理提供初值;对复杂的三维地层采用两个等效处理策略,并为各个等效模型提供多组初值,使得反演过程在速度与精度上得到大幅提升;在后期解释评价中,通过每层地层电阻率各向异性反演结果可精确计算储层含油饱和度、可动油饱和度等,为储层评价提供可靠参数。The beneficial effect of the present invention is that the present invention provides a method for extracting the anisotropic resistivity of horizontal well shale oil reservoirs based on the original signal of array induction well logging, fully utilizes the information of adjacent wells, determines the position of the layer interface, and provides Subsequent processing provides initial values; two equivalent processing strategies are used for complex 3D formations, and multiple sets of initial values are provided for each equivalent model, which greatly improves the speed and accuracy of the inversion process; in the later interpretation and evaluation, Through the inversion results of the resistivity anisotropy of each layer, the reservoir oil saturation, movable oil saturation, etc. can be accurately calculated to provide reliable parameters for reservoir evaluation.

本发明提出的方法可有效消除井斜、围岩和各向异性对测井响应的影响,有效提取水平井页岩油储层的各向异性电阻率信息。The method proposed by the invention can effectively eliminate the influence of well deviation, surrounding rock and anisotropy on the logging response, and effectively extract the anisotropic resistivity information of the shale oil reservoir of the horizontal well.

附图说明Description of drawings

图1为本发明中一种基于阵列感应测井原始信号的水平井页岩油储层各向异性电阻率提取方法流程图;Fig. 1 is a kind of flow chart of the method for extracting the anisotropic resistivity of the horizontal well shale oil reservoir based on the original signal of the array induction logging in the present invention;

图2为本发明等效解释模型示意图;Fig. 2 is a schematic diagram of an equivalent interpretation model of the present invention;

图3为本发明层状各向同性处理模型示意图;Fig. 3 is a schematic diagram of the layered isotropic processing model of the present invention;

图4为本发明均质各向异性处理模型示意图;Fig. 4 is a schematic diagram of the homogeneous anisotropy processing model of the present invention;

图5为本发明65°和80°三层地层模型,其中,(a)为65°三层地层模型,(b)为80°为三层地层模型;Fig. 5 is 65 ° and 80 ° three-layer stratum model of the present invention, wherein, (a) is 65 ° three-layer stratum model, (b) is 80 ° and is three-layer stratum model;

图6为图5模型阵列感应测井各子阵列原始响应,其中,(a)为65°地层模型阵列感应测井各子阵列原始响应,(b)为80°地层模型阵列感应测井各子阵列原始响应;Fig. 6 is the original response of each sub-array of the model array induction logging in Fig. 5, where (a) is the original response of each sub-array of the 65° formation model array induction logging, (b) is the original response of each sub-array of the 80° formation model array induction logging array raw response;

图7为本发明各子阵列所对应的层状各向同性处理模型反演结果,其中,(a)为65°层状各向同性处理模型反演结果,(b)为80°层状各向同性处理模型反演结果;Fig. 7 is the inversion result of the layered isotropic processing model corresponding to each sub-array of the present invention, wherein, (a) is the inversion result of the 65° layered isotropic processing model, (b) is the inversion result of the 80° layered isotropic processing model Isotropic processing model inversion results;

图8为本发明均质各向异性处理模型反演结果,其中,(a)为65°均质各向异性处理模型反演结果,(b)为80°均质各向异性处理模型反演结果。Fig. 8 is the inversion result of the homogeneous anisotropy processing model of the present invention, wherein, (a) is the inversion result of the 65° homogeneous anisotropy processing model, and (b) is the inversion result of the 80° homogeneous anisotropy processing model result.

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The following will clearly and completely describe the technical solutions in the embodiments of the present invention with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only some of the embodiments of the present invention, not all of them. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.

一种水平井页岩油储层各向异性电阻率提取方法,如图1所示,包括如下步骤:A method for extracting the anisotropic resistivity of a horizontal well shale oil reservoir, as shown in Figure 1, comprises the following steps:

s1.获取邻井地层层厚、地层水平电阻率、自然GR曲线信息,以及实测水平井阵列感应测井N个子阵列(SGM0、SGM1……SGMN-1)及合成的视电阻率曲线,其中,水平井阵列感应测井子阵列包括短源距子阵列和长源距子阵列;s1. Obtain the formation thickness, formation horizontal resistivity, and natural GR curve information of adjacent wells, as well as the measured horizontal well array induction logging N sub-arrays (SGM 0 , SGM 1 ... SGM N-1 ) and the synthesized apparent resistivity curves , wherein, the horizontal well array induction logging sub-array includes a short source distance sub-array and a long source distance sub-array;

s2.基于短源距子阵列曲线以及实测水平井GR曲线,划分水平井地层界面;s2. Based on the short source distance sub-array curve and the measured horizontal well GR curve, divide the formation boundary of the horizontal well;

s3.建立解释模型,构建层状各向同性处理模型M1和均质各向异性处理模型M2s3. Establish an interpretation model, construct a layered isotropic processing model M 1 and a homogeneous anisotropic processing model M 2 ;

步骤s3具体包括如下步骤:Step s3 specifically includes the following steps:

s3.1.针对页岩油储层电性特征和钻井环境,考虑井眼、地层褶皱、层厚和井斜影响,建立实际地层模型;s3.1. Based on the electrical characteristics of shale oil reservoirs and the drilling environment, consider the effects of wellbore, formation folds, layer thickness and well deviation, and establish an actual formation model;

s3.2.如图2所示,由于探测范围有限,忽略地层褶皱影响,对步骤s1中N个子阵列信号进行井眼校正后,建立相应的解释模型;s3.2. As shown in Figure 2, due to the limited detection range, the influence of formation folds is ignored, and after borehole correction is performed on the N subarray signals in step s1, a corresponding interpretation model is established;

s3.3.分别考虑层厚和各向异性影响,将地层等效为有层厚影响无各向异性影响地层和有各向异性无层厚影响地层,进而依次构建层状各向同性处理模型M1和均质各向异性处理模型M2s3.3. Considering the influence of layer thickness and anisotropy respectively, the stratum is equivalent to the stratum with thickness influence and no anisotropy influence and the stratum with anisotropy and no thickness influence, and then sequentially builds the layered isotropic processing model M 1 and homogeneous anisotropic processing model M 2 ;

s3.4.如图3所示,层状各向同性处理模型M1包括参数Rtsi、θ和Hj,其中,Rtsi为等效各向同性电阻率,Hj为地层厚度,θ为井斜,i代表第i个子阵列,j代表第j个地层,层状各向同性处理模型M1用于消除层厚影响;s3.4. As shown in Figure 3, the layered isotropic processing model M 1 includes parameters Rts i , θ and H j , where Rts i is the equivalent isotropic resistivity, H j is the formation thickness, and θ is Well deviation, i represents the i-th sub-array, j represents the j-th formation, and the layered isotropic processing model M1 is used to eliminate the influence of layer thickness;

s3.5.如图4所示,均质各向异性处理模型M2包括参数Rhj、θ和Rvj,其中,Rhj为水平电阻率,Rvj为垂向电阻率,θ为井斜,j代表第j个地层,均质各向异性处理模型M2用于获得各向异性信息。s3.5. As shown in Figure 4, the homogeneous anisotropic processing model M 2 includes parameters R hj , θ and R vj , where R hj is the horizontal resistivity, R vj is the vertical resistivity, and θ is the well deviation , j represents the jth formation, and the homogeneous anisotropy processing model M2 is used to obtain anisotropy information.

s4.反演第i个子阵列曲线,获得地层电阻率剖面Rtsi,并将该结果作为下一长源距子阵列的初值;s4. Invert the i-th subarray curve to obtain the formation resistivity profile Rts i , and use this result as the initial value of the next long source distance subarray;

步骤s4具体包括如下步骤:Step s4 specifically includes the following steps:

s4.1.以图5所示地层模型为例,利用邻井参考电阻率、水平井实测子阵列曲线及合成曲线,为资料处理提供反演初值;s4.1. Taking the formation model shown in Figure 5 as an example, use the reference resistivity of adjacent wells, the measured sub-array curves and synthetic curves of horizontal wells to provide initial inversion values for data processing;

s4.2.对第一个子阵列曲线,如图6所示,结合步骤s4.1提供的反演初值与步骤s3中构建的层状各向同性处理模型M1,反演获得地层电阻率剖面Rtsi,并将该结果作为下一个长源距子阵列的初值;s4.2. For the first sub-array curve, as shown in Fig. 6, combined with the inversion initial value provided in step s4.1 and the layered isotropic processing model M 1 constructed in step s3, the formation resistance is obtained by inversion rate profile Rts i , and use this result as the initial value of the next long source distance subarray;

s4.3.对第i个子阵列曲线,将前一子阵列反演得到的地层电阻率剖面Rtsi-1作为反演初值,反演获得地层电阻率剖面Rtsi,并将该结果作为下一长源距子阵列的初值。s4.3. For the ith sub-array curve, use the formation resistivity profile Rts i-1 obtained from the inversion of the previous sub-array as the inversion initial value, invert to obtain the formation resistivity profile Rts i , and use this result as the following The initial value of a long-distance subarray.

s5.如图7所示,依次反演各子阵列视电阻率曲线,分别获得相应的地层电阻率剖面Rtsi,i=1,…,N;s5. As shown in Figure 7, the apparent resistivity curves of each sub-array are inverted sequentially to obtain the corresponding formation resistivity profiles Rts i , i=1,...,N;

s6.对层状各向同性处理模型M1中第j个地层,结合步骤s5的反演结果,采用均质各向异性处理模型M2,反演当前层的各向异性电阻率Rhj和Rvjs6. For the jth formation in the layered isotropic processing model M 1 , combined with the inversion results in step s5, use the homogeneous anisotropic processing model M 2 to invert the anisotropic resistivity R hj and R vj ;

步骤s6具体包括如下步骤:Step s6 specifically includes the following steps:

s6.1.步骤s3建立的均质各向异性处理模型M2,包括参数Rh和Rv,其中,Rh为水平电阻率,Rv为垂向电阻率,该模型忽略层厚影响;s6.1. The homogeneous anisotropy processing model M 2 established in step s3 includes parameters R h and R v , wherein R h is the horizontal resistivity, R v is the vertical resistivity, and this model ignores the influence of layer thickness;

s6.2.如图8所示,对层状各向同性处理模型M1中第j个地层,将步骤s5得到的当前层的N个电阻率剖面作为反演输入信息,结合步骤s3中构建的均质各向异性处理模型M2,对步骤s5的解释结果进行反演,得到当前层的各向异性电阻率Rhj和Rvjs6.2. As shown in Figure 8, for the jth formation in the layered isotropic processing model M1 , the N resistivity profiles of the current layer obtained in step s5 are used as the inversion input information, combined with the construction in step s3 The homogeneous anisotropic processing model M 2 of the step s5 is inverted to obtain the anisotropic resistivity R hj and R vj of the current layer;

s6.3.将层状各向同性处理模型M1中的所有层进行逐层反演,重复上述过程,从而获得各个地层的各向异性电阻率。s6.3. Perform layer-by-layer inversion of all layers in the layered isotropic processing model M1 , and repeat the above process to obtain the anisotropic resistivity of each formation.

s7.依次循环步骤s6,处理层状各向同性处理模型M1中每一层,进而得到各个地层的各向异性电阻率。s7. Step s6 is repeated sequentially to process each layer in the layered isotropic processing model M1 , and then obtain the anisotropic resistivity of each formation.

当然,上述说明并非是对本发明的限制,本发明也并不仅限于上述举例,本技术领域的技术人员在本发明的实质范围内所做出的变化、改型、添加或替换,也应属于本发明的保护范围。Of course, the above descriptions are not intended to limit the present invention, and the present invention is not limited to the above examples. Changes, modifications, additions or replacements made by those skilled in the art within the scope of the present invention shall also belong to the present invention. protection scope of the invention.

Claims (4)

1. A horizontal well shale oil reservoir anisotropic resistivity extraction method is characterized by comprising the following steps:
s1. obtaining the stratum layer thickness, the stratum horizontal resistivity and the natural GR curve information of an adjacent well, and actually measuring N sub-arrays of the horizontal well array induction logging and a synthesized apparent resistivity curve, wherein the horizontal well array induction logging sub-array comprises a short source distance sub-array and a long source distance sub-array;
s2, dividing horizontal well stratum interfaces based on the short source distance subarray curve and an actually measured horizontal well GR curve;
s3. establishes an explanation model and a layered isotropic processing model M 1 And a homogeneous anisotropy processing model M 2
s4. inverses the ith sub-array curve to obtain the formation resistivity profile Rts i And taking the result as an initial value of a next long source distance sub array;
s5. sequentially inverts apparent resistivity curves of the sub-arrays to respectively obtain corresponding formation resistivity profiles Rts i ,i=1,…,N;
s6. model M for layered isotropic processing 1 And (5) combining the inversion result of the step s5 with the jth stratum, and adopting a homogeneous anisotropy processing model M 2 Inverting the anisotropic resistivity R of the current layer hj And R vj
s7. sequentially loops step s6 to process the layered isotropic spotPhysical model M 1 And obtaining the anisotropic resistivity of each stratum.
2. The method for extracting the anisotropic resistivity of the horizontal well shale oil reservoir according to claim 1, wherein the step s3 comprises the following steps:
s3.1, aiming at the electrical characteristics of a shale oil reservoir and the drilling environment, considering the influences of a well hole, stratum folds, layer thickness and well deviation, and establishing an actual stratum model;
s3.2, neglecting stratum fold influence, and establishing a corresponding interpretation model after borehole correction is carried out on the N sub-array signals in the step s 1;
and S3.3, respectively considering the layer thickness and the anisotropic influence, and equating the stratum to a stratum with the layer thickness influence and without the anisotropic influence and a stratum with the anisotropic influence and without the layer thickness influence, and further sequentially constructing a layered isotropic processing model M 1 And a homogeneous anisotropy processing model M 2
S3.4 layered Isotropic treatment model M 1 Including the parameter Rts i Theta and H j Wherein Rts is i For equivalent isotropic resistivity, H j The stratum thickness is shown, theta is well deviation, i represents the ith sub-array, j represents the jth stratum, and the layered isotropic processing model M1 is used for eliminating the layer thickness influence;
s3.5. homogeneous Anisotropic Process model M 2 Comprising a parameter R hj Theta and R vj Wherein R is hj For horizontal resistivity, R vj Homogeneous anisotropy processing model M for vertical resistivity, theta for well deviation, j for jth formation 2 For obtaining anisotropy information.
3. The method for extracting the anisotropic resistivity of the horizontal well shale oil reservoir according to claim 1, wherein the step s4 comprises the following steps:
s4.1, providing an inversion initial value by utilizing the reference resistivity of the adjacent well, the actually measured subarray curve of the horizontal well and the synthetic curve;
s4.2. For the first subarray curve, combine the stepss4.1 and the layered isotropic processing model M constructed in step s3 1 And obtaining formation resistivity profile Rts by inversion i And taking the result as the initial value of the next long-source-distance sub-array;
s4.3, for the ith sub-array curve, performing inversion on the previous sub-array to obtain a formation resistivity profile Rts i-1 As an initial value of inversion, obtaining formation resistivity profile Rts by inversion i And the result is used as the initial value of the next long source range sub-array.
4. The method for extracting the anisotropic resistivity of the horizontal well shale oil reservoir according to claim 1, wherein the step s6 comprises the following steps:
s6.1. homogeneous anisotropy processing model M established in step s3 2 Including a parameter R h And R v Wherein R is h For horizontal resistivity, R v For vertical resistivity, the model ignores layer thickness effects;
s6.2. model M for layer isotropy 1 Taking the N resistivity profiles of the current layer obtained in the step s5 as inversion input information of the jth stratum, and combining the homogeneous anisotropic processing model M constructed in the step s3 2 And (5) inverting the interpretation result of the step s5 to obtain the anisotropic resistivity R of the current layer hj And R vj
S6.3. Model M is treated isotropically in layers 1 And (4) performing layer-by-layer inversion on all the layers, and repeating the process to obtain the anisotropic resistivity of each stratum.
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