Intelligent prediction method and application of single-well in-situ stress in shale reservoirs driven by multi-source data
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摘要: 针对深层页岩具有“高温、高压、高应力及强塑性”的特点,现有地应力测试方法与测井解释模型存在预测精度低、耗时且推广能力弱等缺点,限制了地应力大小解释结果对页岩气勘探开发的有效指导。以川南复杂构造页岩气区块作为典型解剖区,充分利用井点钻、录、测、压裂等各类动、静态多源数据,并结合不同实验条件下的岩石物理参数、岩石力学及地应力大小的测试技术,采用机器学习与地质力学知识双向驱动的方法,构建了多方法融合的地应力大小智能预测方法,并将精细地应力解释剖面应用于页岩气高效开发。龙马溪组一段(龙一段)页岩受有机质含量、矿物组构及围压影响,使得整体下部①—④号小层的各向异性、力学性质及孔隙弹性效应明显强于上部小层。基于这种力学特征的差异,建立了适用于深层页岩的地应力各向同性解释模型。基于实验数据、工程数据及多向标定的地应力解释人工合成数据,形成了川南地区页岩储层地应力标准数据集。采用Pearson因子算法筛选了横波时差、电阻率、声波时差及杨氏模量等敏感特征参数,优化后的轻量级与极限梯度提升混合(L-XGBoost)融合智能模型实现三向地应力大小解释精度均在90%以上,且均方根误差、平均绝对误差及决定系数分别为6.63,3.89及0.91,具有推广泛化应用能力。纵向上受龙一段页岩岩相变化引起的力学强度波动,使其内部发育了4套应力隔挡层,其中①号层顶与⑥号层为2套强应力隔层,储隔应力差大于6 MPa,且褶皱变形挤压应力扰动区局部派生的挤压应力会增强纵向应力的隔挡作用,使得最小水平主应力值变大,造成压裂改造效果变差。研究揭示了龙一段页岩力学各向异性受控地质因素,并据此建立了适用于深层页岩的各向同性地应力解释模型。采用L-XGBoost融合智能模型实现三向地应力预测精度超过90%,明确了龙一段页岩4套应力隔挡层发育特征及其对压裂效果的影响。研究成果将为川东南复杂构造区页岩气纵向开发小层划分和水力压裂优化设计提供科学指导。Abstract:
Objective Deep shale reservoirs are characterized by high temperature, high pressure, elevated in situ stress, and strong plasticity. Conventional in-situ stress testing methods and log interpretation models, often calibrated under simplified laboratory conditions, suffer from limited predictive accuracy, high operational cost, and poor generalizability—challenges that constrain their utility in guiding shale gas exploration and development. Methods Focusing on a structurally complex shale gas block in southern Sichuan as a representative case, we integrated dynamic and static multi-source data across drilling, logging, testing, and production stages. Along with experimental measurements of the physical and mechanical properties of rock under different conditions, we developed a hybrid stress prediction model by combining machine learning techniques with geomechanical principles. This multi-method, log-based intelligent prediction framework enables the generation of high-resolution in-situ stress profiles for efficient shale gas development. Results In the first member of the Longmaxi Formation (Long-1 Member), organic content, confining pressure, and lamination structures significantly influence mechanical anisotropy, particularly in Beds 1–4, which exhibit stronger anisotropy than the upper beds. Based on these findings, we developed a mechanically calibrated anisotropic stress interpretation model for deep shales. Using laboratory- and field-calibrated synthetic stress datasets, we established a standardized stress database for the southern Sichuan shale reservoir. Key sensitive logging parameters, including shear wave slowness, resistivity, acoustic logs, and Young's modulus were identified via Pearson correlation analysis. An optimized XGBoost model achieved interpretation accuracies above 90% for all three principal stress components, with an RMSE of 6.63, an MAE of 3.89, and a coefficient of determination (R2) of 0.91, indicating strong robustness and generalizability. The results revealed four distinct stress barrier layers from the Wufeng Formation to the Longmaxi Formation, and the top of Bed 1 and Bed 6 acted as dominant stress-sealing interfaces. Localized compressive stresses induced by fold-related deformation further enhanced vertical stress compartmentalization and increased the minimum horizontal principal stress, thereby exerting significant influence on hydraulic fracturing performance. Conclusions The study revealed the geological factors controlling the mechanical anisotropy of the shale in the Long-1 Member, and established an isotropic in-situ stress interpretation model suitable for deep shale reservoirs accordingly. An integrated intelligent model, L-XGBoost, was adopted to achieve a prediction accuracy exceeding 90% for three-dimensional in-situ stresses. The research also clarified the development characteristics of four sets of stress barrier layers within the Long-1 Member shale and their impact on fracturing effectiveness. Significance These insights provide a scientific basis for fine-scale stratigraphic subdivision and three-dimensional well pattern design for shale gas development in the tectonically complex southeastern Sichuan Basin. -
图 1 四川盆地构造单元划分及研究区构造特征和地层划分图
a—四川盆地及其周缘构造单元划分图;b—丁山—新场南五峰组—龙马溪组构造特征图;c—DY6-1井五峰组—龙一段页岩开发小层划分与储层综合评价图(硅质含量—测井解释获得的石英和长石含量总和;钙质含量—测井解释获得的方解石与白云石含量总和)
Figure 1. Tectonic framework and stratigraphic division of the Sichuan Basin and the study area
(a) Tectonic subdivision of the Sichuan Basin and adjacent structural units; (b) Structural characteristics of the Wufeng Formation to Longmaxi Formation in the Dingshan–Xinchangnan region; (c) Subdivision and reservoir evaluation of the Wufeng Formation to the first member of the Longmaxi Formation in Well DY6-1(siliceous content—total quartz and feldspar from log interpretation; calcareous content—total calcite and dolomite from log interpretation)
图 2 不同小层岩芯动态与静态Biot系数测试结果及其影响因素分析
a—8组动态Biot系数实验测试结果图;b—页岩孔隙度与Biot系数关系图;c—TOC含量与Biot系数关系图;d—龙一段各小层垂向和水平Biot系数测试差异值关系图;e—纵波速度和横波速度值随有效应力的变化关系图;f—动态和静态Biot系数校正关系模型图
Figure 2. Test results of dynamic and static Biot coefficients for cores from different beds and analysis of their influencing factors
(a) Experimental results from eight groups of dynamic Biot coefficient tests; (b) Relationship between shale porosity and dynamic Biot coefficient; (c) Relationship between total organic carbon (TOC) content and dynamic Biot coefficient; (d) Variations in vertical and horizontal dynamic Biot coefficients across beds of the first member of the Longmaxi Formation; (e) Variation of P-wave and S-wave velocities with effective stress; (f) Correlation between dynamic and static Biot coefficients
图 4 龙马溪组页岩刚度系数矩阵关键参数解释模型构建图
a—参数C12和C13的关系图;b—参数C33和C13+2C44的关系图
Figure 4. Diagram illustrating the construction of the interpretation model for key parameters in the stiffness coefficient matrix of Longmaxi Formation shale
(a) Relationship between parameters C12 and C13; (b) Relationship between parameters C33 and C13+2C44
图 5 垂直和水平方向岩石力学参数动静态转换关系模型图
a—垂直方向弹性模量动、静态转换关系图;b—垂直方向泊松比动、静态转换关系图;c—水平方向弹性模量动、静态转换关系图;d—水平方向泊松比动、静态转换关系图
Figure 5. Dynamic-to-static conversion of mechanical rock parameters of the first member of Longmaxi Formation
(a) Vertical elastic modulus; (b) Vertical Poisson 's ratio; (c) Horizontal elastic modulus; (d) Horizontal Poisson 's ratio
图 6 DYS1井龙一段各模型计算地应力大小结果
DTS—横波时差;DTC—纵波时差;GR—自然伽马;Ev—垂直方向的弹性模量;Eh—水平方向的弹性模量;νv—垂直方向的泊松比;νh—水平方向的泊松比
Figure 6. Variable model-derived in situ stress magnitudes for the first member of Longmaxi Formation at well DYS1
DTS—shear wave slowness; DTC—compressional wave slowness; GR—gamma ray; Ev—vertical Young‘s modulus; Eh—horizontal Young’s modulus; νv—vertical Poisson‘s ratio; νh—horizontal Poisson’s ratio
图 7 岩石力学和地应力与各测井参数之间关系的Pearson热力图
AC—声波时差测井;CNL—补偿中子测井;DEN—体积密度测井;GR—自然伽马测井;RD—深电阻率测井;RS—浅电阻率测井;DTS—横波时差;DTC—纵波时差;DTST—斯通利波时差;Vp—纵波速度;Vs—横波速度;TOC—总有机碳含量a—各岩石力学参数与各类测井参数之间的相关性热力图;b—三向地应力与各类参数之间的相关性热力图
Figure 7. Pearson correlation heatmap between rock mechanical, in-situ stress, and well-logging parameters
(a) Correlation heatmap between rock mechanical parameters and various well-logging parameters; (b) Correlation heatmap between the three principal in situ stresses and various parametersAC—acoustic (slowness) log; CNL—compensated neutron log; DEN—bulk density log; GR—gamma ray log; RD—deep resistivity log; RS—shallow resistivity log; DTS—shear wave slowness; DTC—compressional wave slowness; DTST—stoneley wave slowness; Vp—compressional wave velocity; Vs—shear wave velocity; TOC—total organic carbon
图 9 不同机器学习模型预测三向地应力大小与实测值对比图
a—基于ANN-PSO模型的最大水平地应力大小的预测值与实测值对比图;b—基于ANN-PSO模型的最小水平地应力大小的预测值与实测值对比图;c—基于ANN-PSO模型的垂向地应力大小的预测值与实测值对比图;d—基于LightGBM模型的最大水平地应力大小的预测值与实测值对比图;e—基于LightGBM模型的最小水平地应力大小的预测值与实测值对比图;f—基于LightGBM模型的垂向地应力大小的预测值与实测值对比图;g—基于XGBoost模型的最大水平地应力大小的预测值与实测值对比图;h—基于XGBoost模型的最小水平地应力大小的预测值与实测值对比图;i—基于XGBoost模型的垂向地应力大小的预测值与实测值对比图
Figure 9. Comparison of predicted and measured triaxial in situ stress magnitudes using different machine learning models
(a) Comparison between predicted and measured values of maximum horizontal in situ stress based on the ANN-PSO model; (b) Comparison between predicted and measured values of minimum horizontal in situ stress based on the ANN-PSO model; (c) Comparison between predicted and measured values of vertical in situ stress based on the ANN-PSO model; (d) Comparison between predicted and measured values of maximum horizontal in situ stress based on the LightGBM model; (e) Comparison between predicted and measured values of minimum horizontal in situ stress based on the LightGBM model; (f) Comparison between predicted and measured values of vertical in situ stress based on the LightGBM model; (g) Comparison between predicted and measured values of maximum horizontal in situ stress based on the XGBoost model; (h) Comparison between predicted and measured values of minimum horizontal in situ stress based on the XGBoost model; (i) Comparison between predicted and measured values of vertical in situ stress based on the XGBoost model
图 11 五峰组—龙一段页岩储层不同穿行小层内水力压裂缝上行和下行缝高统计图
a—丁山−东溪地区水平井穿行③号层压裂上、下行缝高占比图;b—丁山−东溪地区水平井穿行②号层压裂上、下行缝高占比图;c—焦石坝地区水平井穿行⑧号层压裂上、下行缝高占比图;d—焦石坝地区水平井穿行⑦号层压裂上、下行缝高占比图
Figure 11. Statistical distribution of upward- and downward-propagating hydraulic fractures within individual beds of the shale reservoir, Wufeng Formation to the Long 1 Member
(a) Proportion of upward vs. downward fracture height in horizontal wells through Bed 3, Dingshan–Dongxi area; (b) Proportion of upward vs. downward fracture height in horizontal wells through Bed 2, Dingshan–Dongxi area; (c) Proportion of upward vs. downward fracture height in horizontal wells through Bed 8, Jiaoshiba area; (d) Proportion of upward vs. downward fracture height in horizontal wells through Bed 7, Jiaoshiba area
图 12 丁山−东溪地区不同构造变形部位纵向应力梯度变化规律及其对储层改造影响分析图
a—中和面不同构造位置关键钻井地应力的梯度变化规律模式图;b—不同构造位置关键井改造体积变化图
Figure 12. Analysis of minimum horizontal principal stress gradient variation patterns across different structural deformation zones in the Dingshan–Dongxi area and their impact on reservoir stimulation
(a) Schematic diagram of gradient variation patterns of in-situ stresses at key drilling locations across different structural positions of the neutral surface; (b) Variation diagram of stimulated reservoir volume for key wells at different structural positions
表 1 丁山—东溪地区龙一段声发射地应力大小测试结果
Table 1. Acoustic emission-based in-situ stress measurements for the first member of Longmaxi Formation in the Dingshan–Dongxi region
井号 深度/m 声发射Kaiser效应点值 最大水平
地应力/MPa最小水平
地应力/MPa垂向地应力/
MPa水力压裂裂缝
闭合压力/MPa0° 45° 90° 垂直 DY1 2045.00 37.45 31.65 36.35 38.51 54.10 43.54 49.76 46.36 DY1 2050.00 40.52 34.65 39.68 38.75 57.52 46.59 50.03 — DY2 4301.00 64.29 54.21 61.75 60.21 121.47 103.67 107.43 — DY2 4320.00 65.15 54.38 61.95 60.12 122.62 104.01 107.55 — DY2 4360.00 66.31 55.08 62.14 59.86 123.83 105.07 107.73 102.56 DY5 3779.42 62.18 51.28 57.91 49.39 107.62 89.58 92.81 91.25 DY6 3444.60 64.18 54.34 57.35 59.12 94.08 79.53 84.70 78.96 DY7 4106.30 55.13 42.72 50.21 47.27 114.04 93.54 100.04 — DY7 4109.49 58.83 46.02 53.08 47.86 117.46 96.77 100.67 97.70 DY7 4115.22 59.18 47.56 54.38 48.23 117.54 98.48 101.11 — DY7 4117.50 60.02 48.05 55.03 48.56 118.58 98.98 101.47 — DY8 4234.07 69.54 55.94 62.31 62.12 123.08 101.84 105.18 105.35 DYS1 4167.20 67.36 55.68 65.21 65.13 113.66 92.34 101.57 — DYS1 4186.36 69.62 58.27 67.03 66.38 115.35 95.07 102.99 — DYS1 4191.45 68.65 56.17 66.80 65.46 116.25 93.06 102.11 — DYS1 4198.10 66.83 56.27 65.53 65.86 113.10 93.24 102.57 — DYS1 4219.30 69.88 56.71 65.59 66.37 116.14 93.68 103.27 93.15 DYS1 4223.72 72.34 59.2 67.61 66.70 118.22 96.16 103.64 — DYS2 4217.31 67.45 54.46 62.18 74.26 119.66 98.29 104.89 101.73 DYS3 4250.00 76.15 67.86 73.59 69.85 117.06 102.81 104.91 103.25 表 2 不同构造单元构造应力系数
Table 2. Statistics of tectonic stress coefficients for different structural units
类型 断凹部位 褶皱窄闭凹部位 斜坡区 断背斜核部 丁山褶皱变形核部 井号 DY2 DY8 DY10 DY6 DYS3 DYS1 DYS2 DYS4 DY7 DY1 DY3 DY15 最大构造应力系数 1.44 1.55 1.53 1.52 1.42 1.35 1.48 1.42 1.31 1.38 1.14 1.20 最小构造应力系数 1.02 1.07 1.16 1.05 0.96 0.86 0.82 0.80 0.80 0.95 0.80 0.64 表 3 各机器学习模型对关键岩石力学与地应力预测效果的评价指标分布统计表
Table 3. Performance metrics of machine learning models for predicting key rock mechanical and in-situ stress parameters
有监督学习
模型评价指标 内聚力/
MPa内摩擦角/
(°)Ⅱ型断裂韧性/
MPa.m1/2泊松比 杨氏模量/
MPa抗压强度/
MPa垂直
主应力/MPa最大水平
主应力/MPa最小水平
主应力/MPaANN-PSO RMSE 1.330 1.878 0.059 0.043 4.538 4.383 12.08 11.89 9.93 MAE 1.006 1.338 0.046 0.038 3.514 3.324 8.64 9.29 7.64 R² 0.880 0.034 0.737 0.055 0.548 0.780 0.56 0.60 0.66 Light
GBMRMSE 0.163 0.116 0.010 0.023 1.567 0.541 9.83 10.70 8.35 MAE 0.731 0.222 0.81 6.630 2.503 0.235 5.91 6.68 5.79 R² 0.998 0.996 0.992 0.831 0.946 0.998 0.75 0.66 0.84 XG
BoostRMSE 0.397 0.217 0.018 0.036 1.809 0.384 8.45 6.32 5.12 MAE 1.88 0.44 1.534 13.930 2.100 0.207 3.57 4.48 3.63 R² 0.989 0.987 0.975 0.342 0.911 0.998 0.85 0.92 0.96 表 4 川南地区五峰组—龙一段页岩储层应力隔层最小水平主应力层间差异值
Table 4. Minimum horizontal principal stress contrast between stress barriers in the Wufeng Formation to Long 1 Member shale reservoir, southern Sichuan Basin
应力隔层位置 应力隔层上/下岩性变化 储隔应力差/MPa(最小值~最大值/平均值) ①号小层与②号小层 观音桥段介壳灰岩强硬层 5.56~9.12/7.86 ③号小层与④号小层 富炭硅质页岩与黏土质页岩 3.52~6.45/5.02 ⑦号小层与⑧号小层 中炭硅质−黏土质页岩与中炭黏土质页岩 4.35~7.42/6.11 ⑤号小层与⑥号小层 高炭硅质−黏土质页岩与中炭硅质−黏土质页岩 6.12~9.36/8.24 -
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