渝东南武隆地区志留系龙马溪组页岩储层的古构造应力场模拟

Simulation of paleotectonic stress field of Silurian Longmaxi shale reservoirs in Wulong area of southeastern Chongqing

  • 摘要: 渝东南武隆地区志留系龙马溪组页岩储层发育,构造裂缝是页岩气运移和聚集的主控因素,而古构造应力场控制着构造裂缝的发育,对武隆地区页岩气的勘探开发具有较大影响。本文对武隆地区及周缘发育的节理进行分期配套处理,明确了武隆地区的古构造应力方向,同时通过岩石声发射实验计算得到了古构造应力的大小。在此基础上,利用ANSYS有限元软件建立了武隆地区志留系龙马溪组地层关键构造变形期的地质模型,并通过构造应力场的分析结果明确了该地区关键构造期的构造应力特征,以确定构造应力场数值模拟的边界条件,进而对构造应力场进行数值模拟。研究结果表明:武隆地区受雪峰陆内造山运动的影响,其主要构造变形期为中燕山中期和中燕山晚期,其中燕山中期的最大、最小水平主应力分别为112—194 MPa和60.93—147.99 MPa,中燕山晚期的最大、最小水平主应力分别为75.67—168.32 MPa和31.19—95.56 MPa。模拟结果显示最大水平主应力的高值区大多集中于武隆西向斜核部、断层上盘的局部区域以及断层的拐点和端点处。页岩气有利保存区与断层上盘的距离要远于断层下盘。向斜的核部曲率越大,越易形成“Λ”型裂缝,越有利于页岩气的储集和保存,因此武隆西向斜的页岩气有利保存区优于武隆东向斜。

     

    Abstract: The development of the shale reservoir within the Silurian Longmaxi Formation in the Wulong area of southeastern Chongqing is significantly affected by the superposition of multiple tectonic processes. This has led to intricate structural deformations in the region, making it imperative to analyze the principal controlling elements for shale gas preservation. Given the shale reservoir’s characteristic low porosity and low permeability, tectonic fractures play a pivotal role as the main controlling factor in the migration and accumulation of shale gas. The paleotectonic stress field determines the development of these tectonic fractures, augmenting the reservoir's storage capacity and enhancing the connectivity among fractures. Consequently, this has a profound impact on the exploration and development of shale gas in the Wulong area. Thus, analyzing the sequence of tectonic evolution, deciphering the direction of the paleotectonic stress field, and quantitatively characterizing the features of the tectonic stress field hold substantial theoretical and practical significance for shale gas exploration and exploitation in this area. In this research paper, comprehensive field measurements were meticulously carried out on the data of conjugate shear joints in the Wulong area and its adjacent periphery. These data were then systematically classified into distinct stages and carefully matched. By leveraging the trend and superposition relationships of fold axes both within the study area and its surrounding regions, the direction of the paleotectonic stress was determined. Through the integration of geochronological data and the outcomes of rock acoustic emission experiments, the tectonic evolution process of the Wulong area was accurately reconstructed. This enabled the determination of the tectonic evolution periods and the corresponding stress magnitudes for each period, while also clarifying the key tectonic deformation period and the fracture distribution traits of the study area. Employing ANSYS finite element software, a three-dimensional geological model was established, specifically focusing on the key tectonic deformation period of the Silurian Longmaxi Formation in the Wulong area. In light of the distribution patterns of rock mechanics parameters in the study area, the mechanics units were appropriately divided, and a corresponding mechanics model was constructed. After multiple rounds of simulation corrections, the optimal boundary stress application conditions for the model were precisely ascertained by analyzing the distinct characteristics of the paleotectonic stress field. Subsequently, numerical simulations of the paleotectonic stress field were executed to elucidate the structural stress characteristics during the key tectonic deformation periods.The research findings reveal that since the middle Yanshanian period, the Wulong area has mainly experienced two phases of structural stress. These phases are characterized by stress directions in the SE−NW orientation and close to the EW direction, with the tectonic stress manifesting as compressive. During the Middle Yanshanian, under the influence of the progressive expansion of the Xuefeng intracontinental orogenic movement from the SE−NW direction, a series of NE-trending faults and associated folds emerged in the Wulong area and its neighboring areas. These formations coalesced to form the primary structural pattern of the Wulong area, marking the principal structural deformation period. This pattern has since become the dominant tectonic configuration in the region. However, during the late stage of Middle Yanshanian, the stress environment generated by the Xuefeng intracontinental orogeny underwent a transformation in the study area. The stress direction shifted from the SE−NW compressive milieu to a near EW compressive stress environment. This led to the formation of near SN-trending faults and related folds in the area, which superimposed upon the pre-existing structural morphology. In the process, L-shaped and T-shaped fold structures materialized in the study area and its environs. Although the tectonic activity during this late stage of Middle Yanshanian did not succeed in changing the main NE-trending tectonic pattern in the Wulong area.Regarding the stress magnitudes, in the middle stage of Middle Yanshanian, the maximum horizontal principal stress ranged from 112 MPa to 194 MPa, while the minimum horizontal principal stress ranged from 60.93 MPa to 147.99 MPa. Notably, the high values of the maximum principal stress were concentrated in the core of the western Wulong syncline. In the late stage of Middle Yanshanian age, the maximum horizontal principal stress fluctuated from 75.67 MPa to 168.32 MPa, and the minimum horizontal principal stress varied from 31.19 MPa to 95.56 MPa. Significantly, the stress value of the western Wulong syncline surpassed that of the eastern syncline. It is also worth noting that there exists a discernible correlation between the stress distribution characteristics and the burial depth. The stress contours were distributed in a ring-like fashion, with the maximum stress value at the central region progressively diminishing outward. Additionally, the stress gradient of the low-value zone exhibited a close relationship with fault intensity. Specifically, the greater the fault intensity, the steeper the stress gradient of the maximum principal stress. The fault zone area functioned as a stress release zone, rendering it a low stress region. At the endpoints and inflection points of the faults, the high stress regions emerged, where stress concentration occurred. Moreover the stress on the hanging wall of the fault was higher than that on the footwall. As a result, the degree of fracture development on the hanging wall of the fault was more pronounced than that on the footwall. Consequently, the favorable preservation area for shale gas was located farther from the hanging wall of the fault compared to the footwall. Moreover, stress concentration at the endpoints and inflection points of the faults led to the relatively developed structural fractures that were easily interconnected, facilitating the escape of shale gas. Hence, these areas were unfavorable for shale gas preservation. Furthermore, the deformation degree of the western Wulong syncline was more pronounced than that of the eastern Wulong syncline. The greater the deformation degree of the syncline, the larger the curvature of its core, making it more susceptible to the formation of ‘Λ’-type fractures. These fractures were conducive to the storage and preservation of shale gas. Therefore, the favorable preservation area for shale gas in the west of the Wulong syncline was superior to that in the east. Studying the characteristics of the paleotectonic stress field lays the foundation for exploring the development degree of tectonic fractures and evaluating the effects of deep fracturing, and it is indeed a critical factor influencing high yields.

     

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