CN111008472A - Discrete element-based splitting basin extension process simulation method - Google Patents

Discrete element-based splitting basin extension process simulation method Download PDF

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CN111008472A
CN111008472A CN201911212834.8A CN201911212834A CN111008472A CN 111008472 A CN111008472 A CN 111008472A CN 201911212834 A CN201911212834 A CN 201911212834A CN 111008472 A CN111008472 A CN 111008472A
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李长圣
尹宏伟
吴珍云
贾东
徐雯峤
汪伟
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Nanjing University
East China Institute of Technology
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Abstract

本发明公开了一种基于离散元的裂谷盆地伸展过程模拟方法,充分考虑地质历史时期地层的地质特征,给出韧性基底构建方法,建立接近裂谷盆地伸展过程的离散元模型。在模拟过程中,可以增加沉积或剥蚀过程,研究这种普遍的地质现象对该区域构造变形的影响。本发明不需要设置先存断层,使模型具有和真实岩体相似的颗粒结构。采用离散元模拟能补充并替换部分实验,而且该基于离散元模拟的构造演化过程与构造变形机制研究方法可以得到实验不容易测得的数据,进而改进现有理论解决实际问题,为裂谷盆地的油气勘探工作提供理论支持。

Figure 201911212834

The invention discloses a method for simulating the extension process of a rift basin based on discrete elements, which fully considers the geological characteristics of the strata in the geological history period, provides a method for constructing a ductile basement, and establishes a discrete element model close to the extension process of the rift basin. During the simulation, deposition or denudation processes can be added to study the effect of this common geological phenomenon on the tectonic deformation of the area. The present invention does not need to set preexisting faults, so that the model has a particle structure similar to the real rock mass. The use of discrete element simulation can supplement and replace some experiments, and the research method of tectonic evolution process and tectonic deformation mechanism based on discrete element simulation can obtain data that is not easy to be measured by experiments, and then improve the existing theory to solve practical problems, which is a good solution for rift basins. Provide theoretical support for oil and gas exploration work.

Figure 201911212834

Description

Discrete element-based splitting basin extension process simulation method
Technical Field
The invention belongs to the technical field of geological structure deformation simulation research, and particularly relates to a discrete element-based method for simulating a valley cracking basin stretching process.
Background
The rift valley basin is formed under the dynamic background of tensile stress, and a great deal of research is carried out on a formation evolution dynamic model of the rift valley basin by predecessors, so that the rift valley basin is a hot spot of oil and gas exploration at home and abroad at present. Through an experimental simulation method, it is necessary to explore the fault formation evolution process of the valley basin under different geological conditions. Moreover, studies have shown that basal lithology controls the pattern of tectonic development within the riflescent valley basin. In constructing a physical simulation, canvas is typically used to simulate a rigid substrate and a blanket to transmit tensile stresses to simulate a flexible substrate.
In the prior art, rigid substrates are mostly adopted for the simulation of the valley cracking basins, but in the nature, the tough substrates exist in the valley cracking basins, and the structural style of the tough substrates is obviously different from that of the valley cracking basins with the rigid substrates. For tough substrates in the valley basin, there is currently a lack of simulation studies.
The discrete element method treats the geologic body as a discrete unit, allows larger relative displacement among particles, can better simulate high deformation, is suitable for the research of discontinuous mechanical behaviors for simulating faults appearing in sedimentary strata and brittle deformation such as fault-related folds and the like, and is an important method for researching a structural deformation process and a deformation mechanism.
Disclosure of Invention
The invention aims to solve the technical problem of providing a discrete element-based method for simulating the stretching process of the valley cracking basin, which realizes the discrete element simulation of the stretching process of the valley cracking basin with a tough substrate and can be used for simulating the fracture evolution process of the valley cracking basin in different substrates.
In order to achieve the purpose of the invention, the following technical scheme is adopted in the application:
a discrete element-based method for simulating a valley cracking basin stretching process comprises the following steps:
1) and extracting stratum information of the area to be analyzed by observing the geology of the area to be analyzed and analyzing seismic data of the area, and inverting the structure evolution process. And carrying out inversion analysis on the seismic analysis graph obtained by analysis to obtain a historical stratigraphic distribution diagram before the valley cracking basin starts to extend, and finally obtaining the historical stratigraphic distribution condition of the area to be analyzed.
2) Constructing a discrete element initial model according to the stratum distribution condition obtained in the step 1): setting the radius of a first particle to be 60m, setting the radius of a second particle to be 80m, and randomly filling the first particle and the second particle into a rectangular box-shaped model with a given size according to a certain proportion, so that the particles are stacked at the bottom of the rectangular box-shaped model under the action of gravity to generate a first discrete element model.
3) And obtaining the mesoscopic parameters of the granular materials of each stratum in the discrete element initial model through a series of biaxial compression experimental tests.
4) Establishing a second discrete element model reflecting the geological characteristics of the area to be analyzed by giving the properties of the granular materials of each stratum according to the stratum distribution condition obtained in the step 1) and the microscopic properties of the granular materials of each stratum obtained in the step 3). The second discrete meta-model comprises a base divided into three parts: a first rigid substrate and a second rigid substrate on both sides and a flexible substrate in the middle. The rigid substrate is limited in particle displacement and rotation, while the flexible substrate is limited in particle displacement and rotation in the vertical direction, so that the particles of the flexible substrate can move freely in the horizontal direction. The toughness substrate and the rigid substrate are bonded, the tensile strength and the shear strength are 1e100 Pa, and the substrate is prevented from being bonded and disconnected.
The tough substrate is composed of mutually overlapped particles, and an initial overlapping rate cratio = | AO |/(rA + rO) is defined, namely the ratio of the circle center distance (| AO |) to the balance distance (rA + rO). When cratio ≦ 0.5, particle A is bonded to particle B across particle O, and in order to avoid the occurrence of the cross-particle bonding, a temporary radius scaling factor rext = r is definedtmp/rold. Temporarily changing the particle radius to r when a bond is createdtmp=roldRext. When cratio =0.4 and rext =0.4, the particle a is just bonded to the particle O after the temporary radius scaling is adopted, and the bonding is avoidedParticle a and particle B produced a bond.
5) Performing iterative operation on the second discrete element model established in the step 4) by adopting a discrete element calculation method to complete simulation of the evolution process of the basin extension structure of the region to be analyzed: setting boundary conditions based on the discrete element model which is obtained in the step 4) and reflects the geological characteristics of the area to be analyzed, fixing the boundaries at the two sides and the substrate, and enabling the boundaries at the two sides and the rigid substrate to be separated at a constant speed, namely giving displacement boundary conditions and simulating the horizontal stretching effect in reality; and adding isomorphic sedimentation to simulate a real geological event.
Further, the microscopic parameters of the particulate material include the following parameters: the radius of the particles, the density of the particles, the shear modulus of the particles, the poisson's ratio of the particles, the coefficient of friction of the particles, the bonding parameters between the particles, the local damping coefficient.
Further, the bonding parameters between the particles were set as follows: the Young modulus measuring amount is 2.0e8 Pa, the shear modulus is 2.0e8 Pa, the tensile strength is 0.0-4.0 e7 Pa, and the shear strength is 0.0-8.0 e7 Pa. The condition for generating the bonding is that | AO | - (rA + rO) ≦ tolerate, wherein tolerate takes 1 e-6.
Furthermore, a Hertz-Mindlin model is adopted as a contact model of the particle material, the radius of the particle is 60m and 80m, the density of the particle is 2500 km/m3, the shear modulus of the particle is 2.9e9 Pa, the Poisson ratio is 0.2, and the local damping coefficient is 0.4. The particle friction coefficient was set to 0.0 during the deposition phase and 0.3 during the extension phase.
The invention discloses a discrete element-based method for simulating a valley basin stretching process, which gives a tough substrate construction method by fully considering the original geological characteristics of a stratum in a geological history period, and establishes a discrete element model close to the geological history period; establishing an initial discrete element model by adopting a mode of randomly distributing particles with different sizes; simulating a certain stage, increasing deposition and denudation events, and researching the influence of general geological phenomena on the structural deformation of the area; according to the invention, a pre-existing fault is not required to be arranged, and the model is constructed by adopting discrete particles, so that the model has a particle structure similar to that of a real rock body; the physical simulation experiment constructed on a large scale is expensive and time-consuming, a part of the experiment can be supplemented and replaced by adopting discrete element simulation, and the data which is not easy to measure in the experiment can be obtained by the structural evolution process and structural deformation mechanism research method based on the discrete element simulation, so that the practical problems of the existing theory solution, such as the structural evolution process and the structural deformation mechanism, stress-strain distribution and the influence thereof on the reservoir property, and the like, are improved, and the theoretical support is provided for the oil-gas exploration work of the valley basin.
Drawings
FIG. 1 is a schematic diagram of the initial overlap ratio of the present invention;
FIG. 2 is a schematic diagram illustrating temporary radius scaling factor definition according to the present invention;
FIG. 3 is a schematic diagram of a substrate generation process in accordance with an embodiment of the present invention;
FIG. 4 is a schematic diagram of a rectangular box of a given size filled with particles randomly according to one embodiment of the present invention;
FIG. 5 is a schematic diagram of two-phase simultaneous structure deposition layers of the discrete element model during the stretching process according to an embodiment of the present invention.
Detailed Description
The following describes in detail a method for simulating a valley splitting basin stretching process based on discrete elements, which is provided by the present invention, with reference to the accompanying drawings. In the description of the present invention, it is to be understood that the terms "left side", "right side", "upper part", "lower part", "bottom", etc., indicate orientations or positional relationships based on those shown in the drawings, and are only for convenience of describing the present invention and simplifying the description, but do not indicate or imply that the device or element referred to must have a specific orientation, be constructed and operated in a specific orientation, "first", "second", etc., do not represent an important degree of the component parts, and thus are not to be construed as limiting the present invention. The specific dimensions used in this example are only for illustrating the technical solution and do not limit the scope of protection of the invention.
A discrete element-based method for simulating a valley cracking basin stretching process comprises the following steps:
1) and extracting stratum information of the area to be analyzed by observing the geology of the area to be analyzed and analyzing seismic data of the area, and inverting the structure evolution process. And carrying out inversion analysis on the seismic analysis graph obtained by analysis to obtain a historical stratigraphic distribution diagram before the valley cracking basin starts to extend, and finally obtaining the historical stratigraphic distribution condition of the area to be analyzed.
2) Constructing a discrete element initial model according to the stratum distribution condition obtained in the step 1): setting the radius of the first particle to be 60m, the radius of the second particle to be 80m, and randomly filling the first particle and the second particle into a rectangular box-shaped model with a given size according to a certain proportion, wherein the proportion can be set as 1: 1. 2: 1. 3: 1, and as shown in fig. 4, are stacked on the bottom of the rectangular box-like model under the action of gravity to generate a first discrete element model.
3) And (3) obtaining the microscopic parameters of the granular materials of each stratum in the discrete element initial model through a series of biaxial compression experiment tests, and simulating the rock deformation of the actual stratum. The microscopic parameters of the particulate material include the following parameters: the radius of the particles, the density of the particles, the shear modulus of the particles, the poisson's ratio of the particles, the coefficient of friction of the particles, the inter-particle bonding parameters, and the like.
The bonding parameters between the particles were set as follows: the Young modulus measuring amount is 2.0e8 Pa, the shear modulus is 2.0e8 Pa, the tensile strength is 0.0-4.0 e7 Pa, and the shear strength is 0.0-8.0 e7 Pa. The condition for generating the bonding is that | AO | - (rA + rO) ≦ tolerate, wherein tolerate takes 1 e-6.
The contact model of the granule material adopts Hertz-Mindlin model, the radius of the granule is 60m and 80m, and the density of the granule is 2500 km/m3The elastic modulus of the particles was 2.9e9 Pa, the Poisson's ratio was 0.2, and the local damping coefficient was 0.4. The particle friction coefficient was set to 0.0 during the deposition phase and 0.3 during the extension phase.
4) Establishing a second discrete element model reflecting the geological characteristics of the area to be analyzed by giving the properties of the granular materials of each stratum according to the stratum distribution condition obtained in the step 1) and the microscopic properties of the granular materials of each stratum obtained in the step 3). As shown in fig. 3, the second discrete meta-model includes a substrate, two sides of the substrate are respectively a left wall and a right wall, and the substrate is divided into three parts: left side rigid base and right side of both sidesA side rigid substrate and a ductile substrate in the middle. The rigid substrate is limited in particle displacement and rotation, while the flexible substrate is limited in particle displacement and rotation in the vertical direction, so that the particles of the flexible substrate can move freely in the horizontal direction. The toughness substrate and the rigid substrate are bonded, the tensile strength and the shear strength are 1e100 Pa, and the substrate is prevented from being bonded and disconnected. In this example, the ductile base is composed of grains overlapped with each other, and an initial overlapping ratio cratio = | AO |/(rA + rO), i.e., a ratio of a circle center distance (| AO |) to an equilibrium distance (rA + rO) is defined. The general range of the initial superposition rate is set to be 0.0-1.0, and the radius scaling coefficient and the initial superposition rate have the same value. When cratio ≦ 0.5, as shown in FIG. 1, particle A is bonded to particle B across particle O, and in order to avoid the occurrence of cross-particle bonding, as shown in FIG. 2, a temporary radius scaling factor rext = r is definedtmp/rold. Temporarily changing the particle radius to r when a bond is createdtmp=roldRext. When cratio =0.4 and rext =0.4, the particle a is just bonded to the particle O after the temporary radius scaling is adopted, and the bonding between the particle a and the particle B is avoided.
5) Performing iterative operation on the second discrete element model established in the step 4) by adopting a discrete element calculation method to complete simulation of the evolution process of the basin extension structure of the region to be analyzed: setting boundary conditions based on the discrete element model which is obtained in the step 4) and reflects the geological characteristics of the area to be analyzed, fixing the boundaries at the two sides and the substrate, and enabling the boundaries at the two sides and the rigid substrate to be separated at a constant speed, namely giving displacement boundary conditions and simulating the horizontal stretching effect in reality; the isomorphic depositional is added to simulate a real geological event, as shown in figure 5. A typical simulation is shown in figure 5. Specifically, a horizontal velocity is applied to the left and right rigid bases and the left and right side walls, with the left and left rigid bases taking-2.0 m/s and the right and right rigid bases taking 2.0 m/s.
Based upon the foregoing description of the preferred embodiment of the invention, it should be apparent that the invention defined by the appended claims is not limited solely to the specific details set forth in the foregoing description, as many apparent variations thereof are possible without departing from the spirit or scope thereof.

Claims (4)

1.一种基于离散元的裂谷盆地伸展过程模拟方法,其特征在于,包括以下步骤:1. a rift basin extension process simulation method based on discrete element, is characterized in that, comprises the following steps: 1)通过观测待分析区域的地质并解析该地区地震资料,提取出待分析区域的地层信息,反演构造演化过程;对解析得到的地震解析图进行反演分析得到裂谷盆地开始伸展前历史地层分布图,最终得到待分析区域伸展前历史地层分布情况;1) By observing the geology of the area to be analyzed and analyzing the seismic data in the area, the stratigraphic information of the area to be analyzed is extracted, and the tectonic evolution process is inverted; the inversion analysis is performed on the seismic analysis map obtained by the analysis to obtain the history of the rift basin before the extension began. Stratigraphic distribution map, and finally get the historical strata distribution before extension in the area to be analyzed; 2)根据步骤1)得到的地层分布情况,构建离散元初始模型:设定第一种颗粒半径为60m,第二种颗粒半径为80m,第一种颗粒和第二种颗粒按照一定的比例随机充填到给定大小的矩形盒状模型中,在重力作用下堆积于该矩形盒状模型中,生成第一离散元模型;2) According to the stratum distribution obtained in step 1), construct the initial discrete element model: set the radius of the first kind of particles to 60m, the radius of the second kind of particles to 80m, and the first kind of particles and the second kind of particles randomly according to a certain proportion Filling into a rectangular box-shaped model of a given size, and accumulating in the rectangular box-shaped model under the action of gravity to generate a first discrete element model; 3)通过一系列双轴压缩实验测试,标定离散元初始模型中各个地层的颗粒材料的细观参数;3) Through a series of biaxial compression experiments, the meso-parameters of granular materials in each formation in the initial discrete element model are calibrated; 4)根据步骤1)得到的地层分布情况及步骤3)得到的各个地层的颗粒材料的微观性质,通过给定各个地层的颗粒材料属性,建立反映待分析区域地质特征的第二离散元模型;所述第二离散元模型包括基底,所述基底分为三个部分:两侧的第一刚性基底和第二刚性基底以及位于中间的韧性基底;对所述刚性基底限制颗粒位移和角速度,而对所述韧性基底则只限制颗粒竖直方向的位移,使韧性基底的颗粒可以在水平方向自由移动;所述韧性基底与刚性基底间产生粘结;4) According to the stratum distribution obtained in step 1) and the microscopic properties of the granular materials of each stratum obtained in step 3), by giving the granular material properties of each stratum, a second discrete element model reflecting the geological characteristics of the area to be analyzed is established; The second discrete element model includes a base that is divided into three parts: a first rigid base and a second rigid base on both sides and a ductile base in the middle; particle displacement and angular velocity are limited to the rigid base, and For the tough substrate, only the vertical displacement of the particles is restricted, so that the particles of the tough substrate can move freely in the horizontal direction; the tough substrate and the rigid substrate are bonded; 所述韧性基底由相互叠合的颗粒组成,定义初始叠合率cratio=|AO|/(rA+rO),即圆心距离(|AO|)与平衡距离(rA+rO)的比值;当cratio≤0.5时,颗粒A跨越颗粒O与颗粒B产生粘结,为了避免出现跨颗粒粘结的情况,定义临时半径缩放系数rext=rtmp/rold;当生成粘结时,将颗粒半径临时改变为rtmp=rold·rext;当cratio=0.4,rext=0.4时,采用临时缩放半径后,颗粒A刚好与颗粒O产生粘结,避免了颗粒A和颗粒B产生粘结;The ductile substrate is composed of overlapping particles, and the initial overlapping ratio cratio=|AO|/(rA+rO) is defined, that is, the ratio of the center distance (|AO|) to the equilibrium distance (rA+rO); when the cratio When ≤0.5, particle A will bond across particle O and particle B. In order to avoid cross-particle bonding, a temporary radius scaling factor rext=r tmp /r old is defined; when bonding is generated, the particle radius is temporarily changed is r tmp =r old ·rext; when cratio=0.4, rext=0.4, after the temporary scaling radius is used, particle A just bonds with particle O, avoiding the bonding between particle A and particle B; 5)对步骤4)建立的第二离散元模型,采用离散元的计算方法进行迭代运算,完成待分析区域盆地伸展构造演化过程模拟:基于步骤4)中得到的反映待分析区域地质特征的离散元模型,设置边界条件,固定两侧边界及基底,使两侧边界和刚性基底匀速分离,即给定位移边界条件,模拟现实中的水平伸展作用;加入同构造沉积,模拟真实地质事件。5) For the second discrete element model established in step 4), the discrete element calculation method is used to perform iterative operations to complete the simulation of the evolution process of the extensional structure of the basin to be analyzed: based on the discrete element obtained in step 4) reflecting the geological characteristics of the area to be analyzed. Meta model, setting boundary conditions, fixing the two sides of the boundary and the base, so that the two sides and the rigid base are separated at a uniform speed, that is, given the displacement boundary conditions, simulate the horizontal extension in reality; add syntectonic deposits to simulate real geological events. 2.根据权利要求1所述的基于离散元的裂谷盆地伸展过程模拟方法,其特征在于,所述颗粒材料的微观性质包括以下参数:颗粒的半径、颗粒的密度、颗粒的剪切模量、颗粒的泊松比、颗粒的摩擦系数、颗粒间的粘结参数、局部阻尼系数。2 . The method for simulating the extension process of a rift basin based on discrete elements according to claim 1 , wherein the microscopic properties of the granular material include the following parameters: the radius of the particle, the density of the particle, the shear modulus of the particle , Poisson's ratio of particles, friction coefficient of particles, bonding parameters between particles, local damping coefficient. 3.根据权利要求2所述的基于离散元的裂谷盆地伸展过程模拟方法,其特征在于,设置颗粒间的粘结参数度如下:剪切模量杨氏模量取2.0e8 Pa,剪切模量2.0e8 Pa,抗拉强度0.0~4.0e7 Pa,剪切强度0.0~8.0e7 Pa;粘结产生的条件为|AO|-(rA+rO)≤tolerate,这里tolerate取1e-6。3. the rift basin extension process simulation method based on discrete element according to claim 2, is characterized in that, setting the bonding parameter degree between particles is as follows: shear modulus Young's modulus is 2.0e8 Pa, shear The modulus is 2.0e8 Pa, the tensile strength is 0.0~4.0e7 Pa, and the shear strength is 0.0~8.0e7 Pa; the condition for bonding is |AO|-(rA+rO)≤tolerate, where tolerate is 1e-6. 4.根据权利要求2所述的基于离散元的裂谷盆地伸展过程模拟方法,其特征在于,所述颗粒材料的接触模型采用Hertz-Mindlin模型,颗粒的密度为2500 km/m3,颗粒的剪切模量为2.9e9 Pa,泊松比为0.2,局部阻尼系数为0.4;沉积阶段,颗粒摩擦系数设为0.0,伸展阶段颗粒摩擦系数设为0.3。4. The method for simulating the extension process of a rift basin based on discrete elements according to claim 2, wherein the contact model of the granular material adopts the Hertz-Mindlin model, the density of the particles is 2500 km/m 3 , the density of the particles is 2500 km/m 3 . The shear modulus was 2.9e9 Pa, the Poisson's ratio was 0.2, and the local damping coefficient was 0.4; the particle friction coefficient was set to 0.0 in the deposition stage and 0.3 in the extension stage.
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