CN115906704A - Single-joint stress-seepage coupling numerical calculation method - Google Patents
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Abstract
Description
技术领域Technical Field
本发明属于流固耦合数值计算领域,特别是涉及一种单节理应力-渗流耦合数值计算方法。The invention belongs to the field of fluid-solid coupling numerical calculation, and in particular relates to a single-joint stress-seepage coupling numerical calculation method.
背景技术Background Art
岩体渗流场与应力场之间存在着耦合作用,位移场、应力场受渗流荷载影响的同时,也影响着岩体中渗流水头的分布,这是由于岩体中分布有众多的节理,应力作用导致节理几何特性发生变化,如节理开度的张开或闭合、节理粗糙性的改变等,从而影响节理的透水性而引起整个岩体渗透性发生重大改变。渗流场的变化会改变渗流力,从而影响节理应力场,两者相互影响。节理渗流和应力耦合是岩石水力学的重要热门课题。There is a coupling effect between the seepage field and the stress field of the rock mass. While the displacement field and the stress field are affected by the seepage load, they also affect the distribution of the seepage head in the rock mass. This is because there are many joints distributed in the rock mass. The stress action causes changes in the geometric characteristics of the joints, such as the opening or closing of the joint opening, the change of the joint roughness, etc., which affects the permeability of the joints and causes a significant change in the permeability of the entire rock mass. Changes in the seepage field will change the seepage force, thereby affecting the joint stress field, and the two affect each other. Joint seepage and stress coupling are important and hot topics in rock hydraulics.
由于岩石节理表面粗糙不平,导致节理应力-渗流耦合机制非常复杂。国内外很多专家学者将节理粗糙度概化成一个或者两个变量来建立应力-渗流耦合模型。这些模型忽略了节理表明细观的凸起体分布和开度分布对应力-渗流耦合机制的影响,从而导致不可避免的误差。为了精确的捕捉节理粗糙度的影响,很多学者采用CFD、离散单元法等数值技术,建立节理的精细化模型,模拟节理应力-渗流耦合过程。然而这种数值模拟方法,需要花大量时间去建立节理离散网格模型,而且数值求解对网格要求高,求解时间长,也经常遇到不收敛问题。因此,CFD模拟应用起来较为麻烦。Due to the roughness of the rock joint surface, the stress-seepage coupling mechanism of the joint is very complicated. Many experts and scholars at home and abroad generalize the joint roughness into one or two variables to establish a stress-seepage coupling model. These models ignore the influence of the microscopic protrusion distribution and the opening distribution of the joint surface on the stress-seepage coupling mechanism, which leads to inevitable errors. In order to accurately capture the influence of joint roughness, many scholars use numerical techniques such as CFD and discrete element method to establish a refined model of the joint and simulate the joint stress-seepage coupling process. However, this numerical simulation method requires a lot of time to establish a discrete grid model of the joint, and the numerical solution has high requirements on the grid, a long solution time, and often encounters non-convergence problems. Therefore, CFD simulation is more troublesome to apply.
发明内容Summary of the invention
本发明的目的是提供一种单节理应力-渗流耦合数值计算方法,以解决上述现有技术存在的对网格要求高和求解时间长问题。The purpose of the present invention is to provide a single joint stress-seepage coupling numerical calculation method to solve the problems of high mesh requirements and long solution time in the above-mentioned prior art.
为实现上述目的,本发明提供了一种单节理应力-渗流耦合数值计算方法,包括以下步骤:To achieve the above object, the present invention provides a single joint stress-seepage coupling numerical calculation method, comprising the following steps:
获取单节理应力-渗流耦合的输入参数,对所述输入参数进行离散化处理,得到离散化单元,其中所述离散化单元包括:接触单元和未接触单元;Obtaining input parameters of single-joint stress-seepage coupling, and discretizing the input parameters to obtain discretized units, wherein the discretized units include: contact units and non-contact units;
基于所述接触单元,建立接触方程,基于所述接触方程,得到接触应力和变形量;Based on the contact unit, a contact equation is established, and based on the contact equation, contact stress and deformation are obtained;
基于所述变形量,对所述未接触单元的开度进行更新,得到更新结果,对所述更新结果进行接触判断,基于判断结果建立未接触单元的雷诺方程,基于所述雷诺方程,得到未接触单元的压力和流速,基于所述压力判断收敛性,若不收敛,则继续建立接触方程,直至收敛为止。Based on the deformation, the opening of the non-contact unit is updated to obtain an updated result, and a contact judgment is performed on the updated result. The Reynolds equation of the non-contact unit is established based on the judgment result. Based on the Reynolds equation, the pressure and flow rate of the non-contact unit are obtained. The convergence is judged based on the pressure. If it does not converge, the contact equation continues to be established until it converges.
优选地,对所述输入参数进行离散化处理的过程包括:Preferably, the process of discretizing the input parameters includes:
获取单节理应力-渗流耦合的输入参数,其中所述输入参数包括:上节理坐标、下节理坐标、高程、初始开度和接触半径,采用矩形单元对上节理和下节理进行离散化处理,得到离散化单元。The input parameters of the single joint stress-seepage coupling are obtained, wherein the input parameters include: upper joint coordinates, lower joint coordinates, elevation, initial opening and contact radius, and the upper joint and the lower joint are discretized by using rectangular units to obtain discretized units.
优选地,所述接触方程包括:作用力平衡方程、变形协调方程和弹性方程。Preferably, the contact equation includes: a force balance equation, a deformation coordination equation and an elasticity equation.
优选地,建立接触方程之前还包括:Preferably, before establishing the contact equation, the following steps are also included:
对所述离散化单元进行初始化判断,判断所述离散化单元是否接触,若接触,则为接触单元;若不接触,则为未接触单元。An initialization judgment is performed on the discretization units to determine whether the discretization units are in contact. If so, the discretization units are contact units; if not, the discretization units are non-contact units.
优选地,得到接触应力和变形量的过程包括:Preferably, the process of obtaining the contact stress and deformation includes:
基于所述作用力平衡方程,采用高斯迭代法对所述作用力平衡方程进行求解,得到凸起体的接触应力和变形量。Based on the force balance equation, the Gaussian iteration method is used to solve the force balance equation to obtain the contact stress and deformation of the protrusion.
优选地,对所述更新结果进行接触判断的过程包括:Preferably, the process of performing contact judgment on the update result includes:
若所述更新结果的开度小于0,则为接触单元;若所述更新结果的开度大于0,则为未接触单元。If the opening degree of the update result is less than 0, it is a contact unit; if the opening degree of the update result is greater than 0, it is a non-contact unit.
优选地,得到未接触单元的压力和流速的过程包括:Preferably, the process of obtaining the pressure and flow rate of the uncontacted unit comprises:
基于所述雷诺方程和立方定律,采用Galerkin法建立雷诺方程的等效弱积分形式,采用双向节点插值的矩形单元建立形函数,基于所述形函数和所述等效弱积分形式,得到每个矩形单元的离散形式和所有未知节点水压力的方程组,基于所述方程组,得到未接触单元的压力和流速。Based on the Reynolds equation and the cubic law, the Galerkin method is used to establish an equivalent weak integral form of the Reynolds equation, and a shape function is established using a rectangular unit with bidirectional node interpolation. Based on the shape function and the equivalent weak integral form, the discrete form of each rectangular unit and a set of equations for all unknown node water pressures are obtained. Based on the set of equations, the pressure and flow rate of the uncontacted units are obtained.
优选地,基于所述压力判断收敛性的过程包括:Preferably, the process of judging convergence based on the pressure includes:
若未接触单元的开度和压力满足收敛性关系式时,则为收敛;若未接触单元的开度和压力不满足收敛性关系式时,则为不收敛。If the opening and pressure of the non-contacting unit satisfy the convergence relationship, it is converged; if the opening and pressure of the non-contacting unit do not satisfy the convergence relationship, it is not converged.
本发明的技术效果为:The technical effects of the present invention are:
本发明提供了一种单节理应力-渗流耦合数值计算方法,获取单节理应力-渗流耦合的输入参数,对所述输入参数进行离散化处理,得到离散化单元,其中所述离散化单元包括:接触单元和未接触单元;基于所述接触单元,建立接触方程,基于所述接触方程,得到接触应力和变形量;基于所述变形量,对所述未接触单元的开度进行更新,得到更新结果,对所述更新结果进行接触判断,基于判断结果建立未接触单元的雷诺方程,基于所述雷诺方程,得到未接触单元的压力和流速,基于所述压力判断收敛性,若不收敛,则继续建立接触方程,直至收敛为止。The present invention provides a single-joint stress-seepage coupling numerical calculation method, which obtains input parameters of the single-joint stress-seepage coupling, discretizes the input parameters to obtain discretized units, wherein the discretized units include: contact units and non-contact units; based on the contact units, a contact equation is established, and based on the contact equation, contact stress and deformation are obtained; based on the deformation, the opening of the non-contact unit is updated to obtain an updated result, contact judgment is performed on the updated result, and a Reynolds equation of the non-contact unit is established based on the judgment result, and the pressure and flow rate of the non-contact unit are obtained based on the Reynolds equation, and convergence is judged based on the pressure. If it does not converge, the contact equation continues to be established until convergence.
本发明能够解决现有技术中对网格要求高、求解时间长和不收敛的技术问题,本发明对某个裂隙进行应力-渗流耦合模拟,得到不同法向应力下开度分布图,流速图和压力图。本发明计算速度快,网格划分简单,划分速度快,实现了电脑自动化处理,本发明考虑了裂隙接触对渗流的影响,使得计算更为合理。The present invention can solve the technical problems of high mesh requirements, long solution time and non-convergence in the prior art. The present invention performs stress-seepage coupling simulation on a certain crack to obtain an opening distribution diagram, a flow velocity diagram and a pressure diagram under different normal stresses. The present invention has a fast calculation speed, simple mesh division, fast division speed, and realizes computer automatic processing. The present invention takes into account the influence of crack contact on seepage, making the calculation more reasonable.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
构成本申请的一部分的附图用来提供对本申请的进一步理解,本申请的示意性实施例及其说明用于解释本申请,并不构成对本申请的不当限定。在附图中:The drawings constituting a part of the present application are used to provide a further understanding of the present application. The illustrative embodiments and descriptions of the present application are used to explain the present application and do not constitute an improper limitation on the present application. In the drawings:
图1为本发明实施例中的计算方法流程图;FIG1 is a flow chart of a calculation method in an embodiment of the present invention;
图2为本发明实施例中的离散裂隙单元接触区域与未接触区域示意图;FIG2 is a schematic diagram of a contact area and a non-contact area of a discrete crack unit in an embodiment of the present invention;
图3为本发明实施例中的劈裂岩块得到裂隙示意图;FIG3 is a schematic diagram of a crack obtained by splitting a rock block in an embodiment of the present invention;
图4为本发明实施例中的裂隙形貌、高程和开度测量示意图;FIG4 is a schematic diagram of the measurement of crack morphology, elevation and opening in an embodiment of the present invention;
图5为本发明实施例中的不用应力下开度分布示意图;FIG5 is a schematic diagram of the opening distribution under no stress in an embodiment of the present invention;
图6为本发明实施例中的不同应力下流速图;FIG6 is a flow velocity diagram under different stresses in an embodiment of the present invention;
图7为本发明实施例中的不同应力下压力分布图。FIG. 7 is a diagram showing pressure distribution under different stresses in an embodiment of the present invention.
具体实施方式DETAILED DESCRIPTION
需要说明的是,在不冲突的情况下,本申请中的实施例及实施例中的特征可以相互组合。下面将参考附图并结合实施例来详细说明本申请。It should be noted that, in the absence of conflict, the embodiments and features in the embodiments of the present application can be combined with each other. The present application will be described in detail below with reference to the accompanying drawings and in combination with the embodiments.
需要说明的是,在附图的流程图示出的步骤可以在诸如一组计算机可执行指令的计算机系统中执行,并且,虽然在流程图中示出了逻辑顺序,但是在某些情况下,可以以不同于此处的顺序执行所示出或描述的步骤。It should be noted that the steps shown in the flowcharts of the accompanying drawings can be executed in a computer system such as a set of computer executable instructions, and that, although a logical order is shown in the flowcharts, in some cases, the steps shown or described can be executed in an order different from that shown here.
实施例一Embodiment 1
如图1所示,本实施例中提供一种单节理应力-渗流耦合数值计算方法,包括:As shown in FIG1 , this embodiment provides a single joint stress-seepage coupling numerical calculation method, including:
S1.输入参数:分别输入上下节理坐标(x,y)和高度h(x,y)S1. Input parameters: input upper and lower joint coordinates (x, y) and height h (x, y) respectively
S2.离散化处理:采用矩形单元对上下节理进行离散化处理,每个单元记为(i,j),如图2所示。S2. Discretization: The upper and lower joints are discretized using rectangular units, and each unit is denoted as (i, j), as shown in Figure 2.
S3.初始化判断:判断每个单元是否接触,接触单元记为(i,j)m,未接触单元记为(i,j)n S3. Initialization judgment: judge whether each unit is in contact, the contact unit is recorded as (i,j) m , and the non-contact unit is recorded as (i,j) n
S4.建立接触区域(i,j)m的作用力平衡方程、变形协调方程和弹性方程并进行求解,得到接触单元力的大小和位移大小。S4. Establish the force balance equation, deformation coordination equation and elastic equation of the contact area (i, j) m and solve them to obtain the magnitude of the contact unit force and displacement.
力的平衡方程如下:The force balance equation is as follows:
其中F(i,j)m为应力分布,P(i,j)n为孔隙水压力分布,R1(i,j)为上节理半径,R2(i,j)为下节理半径,见图2,R为凸起体等效半径,R=(R1(i,j)+R2(i,j))/2,Δu为变形量,v为流速。Where F(i,j) m is the stress distribution, P(i,j) n is the pore water pressure distribution, R1 (i,j) is the upper joint radius, R2 (i,j) is the lower joint radius, see Figure 2, R is the equivalent radius of the protrusion, R = ( R1 (i,j) + R2 (i,j))/2, Δu is the deformation, and v is the flow velocity.
对于力的平衡方程组,采用高斯迭代法进行求解,可得到凸起体的应力分布F(i,j)m和变形量Δu。The Gaussian iteration method is used to solve the force balance equations to obtain the stress distribution F(i,j) m and deformation Δu of the protrusion.
S5.根据上一步得到变形值Δu利用开度计算公式对未接触区域的开度b(i,j)n进行更新。S5. Based on the deformation value Δu obtained in the previous step, the opening b(i, j) n of the non-contact area is updated using the opening calculation formula.
开度计算公式如下:The calculation formula of opening is as follows:
b(i,j)n=b(i,j)n-Δuk (2)b(i,j) n =b(i,j) n -Δu k (2)
S6.根据计算出的结果判断每个单元是否接触:若b(i,j)n<0,则单元接触,记为(i,j)m,开度为0;若b(i,j)n>0,则单元未接触,未接触单元记为(i,j)n S6. Determine whether each unit is in contact based on the calculated results: if b(i,j) n < 0, the unit is in contact, recorded as (i,j) m , and the opening is 0; if b(i,j)n> 0, the unit is not in contact, and the non-contact unit is recorded as (i,j) n
S7.建立未接触单元(i,j)n的雷诺方程离散化的整体传导方程并对其求解,得到未接触区域的压力与流速大小。S7. Establish the overall conduction equation of the discretization of the Reynolds equation of the non-contact unit (i, j) n and solve it to obtain the pressure and flow velocity in the non-contact area.
考虑水流满足雷诺方程和立方定律,雷诺方程和立方定律为:Considering that the water flow satisfies the Reynolds equation and the cubic law, the Reynolds equation and the cubic law are:
采用Galerkin法建立雷诺方程的等效弱积分形式:The Galerkin method is used to establish the equivalent weak integral form of the Reynolds equation:
采用双向节点插值的矩形单元建立形函数:The shape functions are created using rectangular elements with bidirectional node interpolation:
式(6)带入式(5)中,得到每个矩形单元的离散形式,Substituting equation (6) into equation (5), we get the discrete form of each rectangular unit:
KePe=Fe (7) KePe = Fe (7)
将单元矩阵中相应编号的系数相加,即可形成式(5)中的总传导矩阵,并得到求解所有未知节点水压力的方程组:By adding the coefficients of the corresponding numbers in the unit matrix, the total conduction matrix in equation (5) can be formed, and the equation system for solving the water pressure of all unknown nodes can be obtained:
KP=F (11)KP=F (11)
其中,[K]的元素常数项采用预处理共轭梯度法对式(11)进行求解,得到未接触区域单元上的水压力Among them, the elements of [K] Constant term The preconditioned conjugate gradient method is used to solve equation (11) to obtain the water pressure on the uncontacted area unit:
S8.求解出未接触单元的压力值P(i,j)m S8. Solve for the pressure value of the uncontacted unit P(i,j) m
S9.判断是否收敛:若||bk-bk+1||<1e-4,||Pk-Pk+1||<1e-4则收敛,计算完成,其中bk和bk+1分别表示未接触单元的k和k+1迭代步的开度大小,Pk和Pk+1分别表示未接触单元的k和k+1迭代步的压力大小;S9. Determine whether it converges: if ||b k -b k+1 ||<1e-4, ||P k -P k+1 ||<1e-4, then it converges and the calculation is completed, where b k and b k+1 represent the opening sizes of the k and k+1 iteration steps of the non-contact unit, respectively, and P k and P k+1 represent the pressure sizes of the k and k+1 iteration steps of the non-contact unit, respectively;
若不收敛,更新接触单元与未接触单元的F(i,j)m与P(i,j)n,再次建立接触单元的作用力平衡方程、变形协调方程和弹性方程并求解,得到接触单元力和变形大小,重复S5-S8,直至收敛为止。If it does not converge, update F(i,j) m and P(i,j) n of the contact unit and the non-contact unit, establish the force balance equation, deformation coordination equation and elastic equation of the contact unit again and solve them to obtain the contact unit force and deformation, and repeat S5-S8 until convergence.
S10.结束计算。S10. End calculation.
具体实施案例如下:The specific implementation cases are as follows:
①首先将150mm×150mm×150mm花岗岩试件进行巴西劈裂以获取新鲜完整裂隙,如图3所示;① First, the 150mm×150mm×150mm granite specimen was Brazilian split to obtain fresh and complete cracks, as shown in Figure 3;
②裂隙形貌数据测量、初始开度和接触半径测量。首先在上、下裂隙试件四个侧面黏贴标记点(如图4所示),用三维光学扫描系统分别扫描上、下裂隙粗糙面和“闭合”下的轮廓,获得点云数据;然后将其导入Geomaic studio软件中,运用软件的“拼接”功能,匹配上、下裂隙标记点,“模拟”裂隙闭合状态(图4);最后取出上、下裂隙面,计算得到上下形貌高程,然后上下节理高程相减,得到闭合裂隙初始开度分布数据,如果某点上节理减去下节理小于0,说明接触,那么这点开度为0。接触半径以上或者下节理最低高程,通过每点减最低高程,得到接触半径值。②Measurement of crack morphology data, initial opening and contact radius. First, stick marking points on the four sides of the upper and lower crack specimens (as shown in Figure 4), and use a three-dimensional optical scanning system to scan the upper and lower crack rough surfaces and the contours under the "closure" to obtain point cloud data; then import it into the Geomaic studio software, use the "stitching" function of the software to match the upper and lower crack marking points, and "simulate" the crack closure state (Figure 4); finally, take out the upper and lower crack surfaces, calculate the upper and lower morphological elevations, and then subtract the upper and lower joint elevations to obtain the initial opening distribution data of the closed crack. If the upper joint minus the lower joint at a certain point is less than 0, it means contact, and the opening at this point is 0. The lowest elevation of the joint above or below the contact radius is obtained by subtracting the lowest elevation from each point to obtain the contact radius value.
③输入参数和离散化处理:分别输入上下节理坐标(x,y),高程h(x,y),初始开度b(i,j),接触半径R1(x,y)和R2(x,y)。采用矩形单元对上下节理进行离散化处理,每个单元记为(i,j),如图2所示。③ Input parameters and discretization: Input the upper and lower joint coordinates (x, y), elevation h(x, y), initial opening b(i, j), contact radius R 1 (x, y) and R 2 (x, y) respectively. Use rectangular units to discretize the upper and lower joints, and each unit is recorded as (i, j), as shown in Figure 2.
④初始化判断:判断每个单元是否接触,接触单元记为(i,j)m,未接触单元记为(i,j)n ④ Initialization judgment: judge whether each unit is in contact, the contact unit is recorded as (i,j) m , and the non-contact unit is recorded as (i,j) n
⑤建立接触区域(i,j)m的作用力平衡方程、变形协调方程和弹性方程并进行求解,得到接触单元力的大小和位移大小。同时更新新的开度值并判断是否接触。⑤ Establish and solve the force balance equation, deformation coordination equation and elastic equation of the contact area (i, j) m to obtain the magnitude of the contact unit force and displacement. At the same time, update the new opening value and determine whether there is contact.
⑥建立未接触单元(i,j)n的雷诺方程离散化的整体传导方程并对其求解,得到未接触区域的压力与流速大小。并求解出未接触单元的压力值。⑥ Establish the overall conduction equation of the discretization of the Reynolds equation of the non-contact unit (i, j) n and solve it to obtain the pressure and flow velocity of the non-contact area. And solve the pressure value of the non-contact unit.
⑦判断是否收敛:若||bk-bk+1||<1e-4,||Pk-Pk+1||<1e-4则收敛,计算完成;若不收敛,更新接触单元与未接触单元的F(i,j)m与P(i,j)n,再次建立接触单元的作用力平衡方程、变形协调方程和弹性方程并求解,得到接触单元力和变形大小,重复⑤-⑦,直至收敛为止。⑦ Determine whether it converges: If ||b k -b k+1 ||<1e-4, ||P k -P k+1 ||<1e-4, it converges and the calculation is completed; if it does not converge, update F(i,j) m and P(i,j) n of the contact unit and the non-contact unit, establish the force balance equation, deformation coordination equation and elastic equation of the contact unit again and solve them to obtain the contact unit force and deformation, repeat ⑤-⑦ until convergence.
⑧结束计算。⑧End the calculation.
⑨设置不同压力重新计算变形和渗流。本次计算用的法向应力分别为:0、1、2、3、4和5MPa。图5、图6和图7分别为不同法向应力下开度、流速和压力分布。⑨ Set different pressures to recalculate deformation and seepage. The normal stresses used in this calculation are: 0, 1, 2, 3, 4 and 5 MPa. Figures 5, 6 and 7 show the opening, flow rate and pressure distribution under different normal stresses.
本实施例有益效果:Beneficial effects of this embodiment:
本实施例能够解决现有技术中对网格要求高、求解时间长和不收敛的技术问题,本实施例对某个裂隙进行应力-渗流耦合模拟,得到不同法向应力下开度分布图,流速图和压力图。本实施例计算速度快,网格划分简单,划分速度快,实现了电脑自动化处理,本实施例考虑了裂隙接触对渗流的影响,使得计算更为合理。This embodiment can solve the technical problems of high mesh requirements, long solution time and non-convergence in the prior art. This embodiment performs stress-seepage coupling simulation on a certain crack to obtain the opening distribution diagram, flow velocity diagram and pressure diagram under different normal stresses. This embodiment has fast calculation speed, simple mesh division, fast division speed, and realizes computer automatic processing. This embodiment takes into account the influence of crack contact on seepage, making the calculation more reasonable.
以上所述,仅为本申请较佳的具体实施方式,但本申请的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本申请揭露的技术范围内,可轻易想到的变化或替换,都应涵盖在本申请的保护范围之内。因此,本申请的保护范围应该以权利要求的保护范围为准。The above is only a preferred specific implementation of the present application, but the protection scope of the present application is not limited thereto. Any changes or substitutions that can be easily thought of by a person skilled in the art within the technical scope disclosed in the present application should be included in the protection scope of the present application. Therefore, the protection scope of the present application should be based on the protection scope of the claims.
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