CN111666620A - Quantitative description method for lateral pressure distribution characteristics of granular material - Google Patents

Quantitative description method for lateral pressure distribution characteristics of granular material Download PDF

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CN111666620A
CN111666620A CN202010466314.6A CN202010466314A CN111666620A CN 111666620 A CN111666620 A CN 111666620A CN 202010466314 A CN202010466314 A CN 202010466314A CN 111666620 A CN111666620 A CN 111666620A
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lateral pressure
pressure distribution
distribution
granular material
intensity
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CN111666620B (en
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来志强
江恩慧
王仲梅
赵连军
徐梓曜
徐阳
梅锐锋
任棐
武彩萍
吴国英
高梓轩
樊科伟
王嘉仪
潘丽
张文皎
王远见
李军华
张向萍
许琳娟
张敏
来嘉豪
来亮
张清清
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Abstract

The invention relates to a parameter determination method in hydraulic design, in particular to a parameter determination method for quantitatively describing the lateral pressure distribution characteristics of a granular material, belonging to a general method in the field of hydraulic engineering, wherein the IPC classification number of the method is E02B 1/00. The method of the invention definitely aims at the measuring size value range for describing the lateral pressure characteristics of the granular material, accurately determines the numerical values of two parameters of the lateral pressure action position concentration and the distribution intensity fluctuation, quantitatively describes the lateral pressure distribution characteristics, can truly reflect the discrete characteristics of the lateral pressure distribution of the granular material, can guide engineering designers to more accurately determine the pressure distribution during the engineering design of retaining walls, foundation pits, deep-buried tunnels and the like, and ensures the engineering safety.

Description

一种颗粒材料侧向压力分布特征定量描述方法A Quantitative Description Method of Lateral Pressure Distribution Characteristics of Granular Materials

技术领域technical field

本发明涉及一种水工设计时的参数确定方法,具体涉及一种定量描述颗粒材料侧向压力分布特征的参数的确定方法,属于水利工程领域的一般方法,其 IPC分类号为E02B1/00。The invention relates to a method for determining parameters in hydraulic design, in particular to a method for determining parameters quantitatively describing lateral pressure distribution characteristics of granular materials, which belongs to a general method in the field of hydraulic engineering, and whose IPC classification number is E02B1/00.

背景技术Background technique

水库大坝工程中常见的颗粒材料有筑坝材料堆石体、土体、泥沙等。这些颗粒材料因自重或外荷载作用下会产生侧向压力,在高堆石坝、挡土墙、深埋隧道等工程建设时必须加以考虑。特别是有关土石侧向压力问题的研究已有200 多年历史,目前工程上常用的侧向压力计算理论是朗肯和库伦土压力理论。两大经典理论均假定侧向压力沿土石体等颗粒材料的堆积深度呈线性分布。侧向压力为线性分布的假定在国内外挡土墙设计规范、基坑结构稳定分析及深埋隧道等工程领域广泛使用。The common granular materials in reservoir dam engineering are rockfill, soil, sediment and so on. These granular materials will generate lateral pressure due to their own weight or external loads, which must be considered in the construction of high rockfill dams, retaining walls, deep tunnels and other projects. In particular, the research on the lateral pressure of soil and rock has a history of more than 200 years. At present, the commonly used lateral pressure calculation theory in engineering is the Rankine and Coulomb soil pressure theory. Both classical theories assume that the lateral pressure is linearly distributed along the accumulation depth of granular materials such as soil and rock. The assumption that lateral pressure is linearly distributed is widely used in engineering fields such as retaining wall design specifications, foundation pit structural stability analysis, and deep tunnels.

然而,土石等工程材料是非常复杂的颗粒材料,传统的宏观连续介质理论往往忽略了对其离散特性的考虑。近年来,离散单元法(Discrete Element Method, DEM)的发展和计算机性能的飞速提高,使得通过细观数值方法研究土石等颗粒材料的力学行为特性成为可能。目前,已有的离散元数值模拟[1-3]研究表明,土石等颗粒材料堆积后将导致拱结构效应的存在,这使得颗粒材料的侧向压力呈现非线性分布(折线型分布),部分侧向压力值相比于线性分布的设计值骤增,这将十分不利于工程安全。However, engineering materials such as earth and rock are very complex granular materials, and the traditional macroscopic continuum theory often ignores the consideration of their discrete properties. In recent years, the development of Discrete Element Method (DEM) and the rapid improvement of computer performance have made it possible to study the mechanical behavior characteristics of granular materials such as soil and rock through mesoscopic numerical methods. At present, the existing discrete element numerical simulation [1-3] studies have shown that the accumulation of granular materials such as soil and stone will lead to the existence of the arch structure effect, which makes the lateral pressure of the granular materials present a nonlinear distribution (polygonal distribution), and some Compared with the design value of linear distribution, the lateral pressure value increases sharply, which will be very detrimental to engineering safety.

当颗粒材料作用于挡墙某些部位的侧向压力过多以及压力强度变化剧烈时,在应力集中作用下挡墙较易失稳坍塌。因此,研究侧向压力作用位置密集度和分布强度波动性性对工程设计安全具有十分重要的意义。但是,目前还没有对颗粒材料侧向压力分布位置密集度和分布强度波动性定量描述方法的相关文献及报道。When the lateral pressure exerted by the granular material on some parts of the retaining wall is too large and the pressure intensity changes drastically, the retaining wall is more prone to instability and collapse under the action of stress concentration. Therefore, it is of great significance for the safety of engineering design to study the fluctuation of the location density and distribution intensity of lateral pressure. However, there are no relevant literatures and reports on the quantitative description method of the position density and distribution intensity fluctuation of the lateral pressure distribution of granular materials.

以下给出检索出的相关文献:The relevant papers retrieved are listed below:

[1]孟云伟等.石笼挡土墙的颗粒离散元细观力学模拟研究[J].岩土力学,2010,31(8):2677-2681.[1] Meng Yunwei et al. Study on particle discrete element meso-mechanical simulation of gabion retaining wall [J]. Geotechnical Mechanics, 2010, 31(8): 2677-2681.

[2]刘冬等.基于DEM分析的有限宽度填土主动土压力计算[J].公路工程,2019,44(02):36-40.[2] Liu Dong et al. Calculation of active earth pressure for finite-width fill based on DEM analysis [J]. Highway Engineering, 2019, 44(02): 36-40.

[3]万励等.无黏性有限土体主动破坏及土压力离散元分析[J].土木与环境工程学报(中英文),2019,41(03):22-29.[3] Wan Li et al. Active failure of incohesive finite soil and discrete element analysis of earth pressure [J]. Chinese and English Journal of Civil and Environmental Engineering, 2019, 41(03): 22-29.

[4]瞿波.分形几何与流体[M].上海:上海社会科学院出版社,2014:3-14.[4] Qu Bo. Fractal geometry and fluid [M]. Shanghai: Shanghai Academy of Social Sciences Press, 2014: 3-14.

发明内容SUMMARY OF THE INVENTION

本发明是为了解决上述问题而进行的,目的是提供一种颗粒材料侧向压力分布特征定量描述方法。本发明方法简单有效,参数的物理意义明确,能够客观准确地量化颗粒材料侧向压力分布位置密集度和分布强度的波动性。The present invention is made to solve the above-mentioned problems, and the purpose is to provide a quantitative description method for the lateral pressure distribution characteristics of granular materials. The method of the invention is simple and effective, the physical meaning of the parameters is clear, and the fluctuation of the distribution position density and distribution intensity of the lateral pressure of the granular material can be objectively and accurately quantified.

本发明的一种颗粒材料侧向压力分布特征定量描述方法,包括以下步骤:A method for quantitatively describing the lateral pressure distribution characteristics of granular materials of the present invention includes the following steps:

步骤1,选取颗粒材料侧向压力分布位置密集度测量尺度:测量确定颗粒材料堆积稳定后的高度H0(单位为m),选取一系列测量尺度参数 ri(i=1,2,…n),其中r1满足

Figure BSA0000210039260000021
的条件。Step 1, select the measurement scale of the position density of the lateral pressure distribution of the granular material: measure the height H 0 (unit is m) after the stable accumulation of the granular material is determined, and select a series of measurement scale parameters r i (i=1, 2, ... n ), where r 1 satisfies
Figure BSA0000210039260000021
conditions of.

步骤2,获取不同测量尺度下侧向压力分布位置密集度的测量数目:测量尺度ro将挡墙平均划分成数目为

Figure BSA0000210039260000022
间距长度为ri的子组,统计子组中含有侧向压力作用点的子组数目ni。Step 2: Obtain the number of measurements of the location density of lateral pressure distribution under different measurement scales: The measurement scale r o divides the retaining wall equally into the number of
Figure BSA0000210039260000022
For the subgroups whose spacing length is ri, count the number of subgroups ni that contain the action points of lateral pressure in the subgroups.

步骤3,求取描述侧向压力分布位置密集度参数d:将步骤2得到的一系列 ri和相应的ni绘制于双对数坐标系中,拟合logri与logni之间的线性关系,得到其可决系数R2,当R2大于0.8时,此时拟合直线斜率的绝对值即侧向压力分布位置密集度参数d。Step 3, find the density parameter d describing the lateral pressure distribution: draw a series of ri and corresponding ni obtained in step 2 in a double logarithmic coordinate system, and fit the linear relationship between logr i and logn i relationship to obtain its coefficient of determination R 2 . When R 2 is greater than 0.8, the absolute value of the slope of the fitted straight line is the position density parameter d of the lateral pressure distribution.

颗粒材料侧向压力分布位置密集度参数d为0~1之间数值,0表示作用位置分布几乎集中在某一点处,1则表示作用位置分布为线性连续分布。d越大,表明颗粒材料侧向压力分布位置越分散。The position density parameter d of the lateral pressure distribution of granular materials is a value between 0 and 1. 0 means that the action position distribution is almost concentrated at a certain point, and 1 means that the action position distribution is a linear continuous distribution. The larger the d is, the more dispersed the lateral pressure distribution position of the particulate material is.

步骤4,选取颗粒材料侧向压力分布强度波动性测量尺度:绘制颗粒材料侧向压力分布图,定义侧向压力折线的上、下两个端点分别为Pup和Pdown,选取一系列尺度参数Ri(i=1,2,…n),其中Ri满足

Figure BSA0000210039260000031
的条件。Step 4: Select the measurement scale for the fluctuation of the lateral pressure distribution intensity of the granular material: draw the lateral pressure distribution diagram of the granular material, define the upper and lower endpoints of the lateral pressure polyline as P up and P down , and select a series of scale parameters Ri ( i =1, 2,... n ), where Ri satisfies
Figure BSA0000210039260000031
conditions of.

步骤5,获取不同测量尺度下侧向压力分布强度波动性的测量数目:以颗粒材料侧向压力分布折线上端点Pup为圆心,以Ri为半径画圆,所述的圆与侧向压力分布折线相交于点P1;然后,再以点P1为圆心,以Ri为半径画圆,与侧向压力分布折线相交于点P2;以此类推,当交点Pn与Pdown在侧向压力分布折线上的距离l小于或等于Ri时,测量结束,最终得到以Ri为尺度量取侧向压力分布折线的数目Ni=n+l/RiStep 5: Obtain the number of measurements of the intensity fluctuation of the lateral pressure distribution under different measurement scales: take the endpoint P up on the broken line of the lateral pressure distribution of the granular material as the center of the circle, and draw a circle with R i as the radius, and the circle is related to the lateral pressure. The distribution polyline intersects at point P 1 ; then, draw a circle with point P 1 as the center and R i as the radius, and intersect the lateral pressure distribution polyline at point P 2 ; and so on, when the intersection points P n and P down are at When the distance l on the lateral pressure distribution broken line is less than or equal to R i , the measurement ends, and finally the number of lateral pressure distribution broken lines measured with R i as the scale N i =n+l/R i is obtained.

步骤6,求取描述侧向压力分布强度波动性参数。将步骤5得到一系列Ri和相应的Ni绘制于双对数坐标系中,拟合logRi与logNi之间的线性函数关系,得到其可决系数R2;当拟合函数的可决系数R2大于0.8时,此时拟合直线斜率的绝对值即侧向压力分布强度波动性参数D。Step 6: Obtain parameters describing the fluctuation of lateral pressure distribution intensity. Draw a series of R i and corresponding N i obtained in step 5 in the double logarithmic coordinate system, and fit the linear function relationship between logR i and logN i to obtain its coefficient of determination R 2 ; When the coefficient of determination R 2 is greater than 0.8, the absolute value of the slope of the fitted straight line is the lateral pressure distribution intensity fluctuation parameter D.

颗粒材料侧向压力分布强度波动性参数D值在1~2之间,1表示侧向压力强度分布为直线分布,2则表示侧向压力强度分布为平面分布。D越大表明侧向压力分布强度波动性越大,拱结构效应越明显,侧向压力骤增点越多。The value of the fluctuation parameter D of the lateral pressure distribution intensity of granular materials is between 1 and 2. 1 means that the lateral pressure intensity distribution is a linear distribution, and 2 means that the lateral pressure intensity distribution is a plane distribution. The larger the D, the greater the fluctuation of the lateral pressure distribution intensity, the more obvious the arch structure effect, and the more the lateral pressure sudden increase points.

与现有的技术相比,本发明的优势效果在于:Compared with the prior art, the advantages of the present invention are as follows:

传统土压力理论基于连续介质假定,这有悖于土石等颗粒材料离散特性的本质,对颗粒材料侧向压力分布特性的描述不准确。本发明改进分形理论思想,选取颗粒材料侧向压力分布特征的测量尺度取值范围,精确确定侧向压力作用位置密集度和分布强度波动性两个参数的数值,对侧向压力分布特征进行定量描述,能够真实反映出颗粒材料侧向压力分布的离散特征,可以指导工程设计人员在挡墙、基坑、深埋隧道等工程设计时更精确地确定压力分布,保证工程安全。The traditional earth pressure theory is based on the assumption of continuum, which is contrary to the nature of discrete characteristics of granular materials such as soil and rock, and the description of the lateral pressure distribution characteristics of granular materials is inaccurate. The invention improves the idea of fractal theory, selects the measurement scale value range of the lateral pressure distribution characteristics of granular materials, accurately determines the values of two parameters, the density of the lateral pressure action position and the fluctuation of the distribution intensity, and quantifies the lateral pressure distribution characteristics. The description can truly reflect the discrete characteristics of the lateral pressure distribution of granular materials, and can guide engineering designers to more accurately determine the pressure distribution in the design of retaining walls, foundation pits, deep tunnels and other projects to ensure project safety.

附图说明Description of drawings

图1是颗粒材料侧向压力分布位置密集度定量描述方法示意图;Figure 1 is a schematic diagram of a method for quantitatively describing the location density of the lateral pressure distribution of granular materials;

图2是颗粒材料侧向压力分布强度波动性定量描述方法示意图;Figure 2 is a schematic diagram of a quantitative description method for the fluctuation of the lateral pressure distribution intensity of granular materials;

图3是采用DEM数值模拟堆积稳定后的颗粒材料;Figure 3 is the granular material after DEM numerical simulation is used to stabilize the accumulation;

图4是颗粒粒径s为0.01m、颗粒摩擦系数μ为0.30条件下侧向压力分布图(a)以及分布强度波动性分析图(b)~图(e);Figure 4 is the lateral pressure distribution diagram (a) and the distribution intensity fluctuation analysis diagrams (b) to (e) under the condition that the particle size s is 0.01 m and the particle friction coefficient μ is 0.30;

图5是不同颗粒粒径和颗粒摩擦系数条件下侧向压力分布位置密集度定量描述中ri与ni拟合函数关系;Figure 5 is the fitting function relationship between ri and ni in the quantitative description of the positional density of lateral pressure distribution under the conditions of different particle sizes and particle friction coefficients;

图6是不同颗粒粒径和颗粒摩擦系数条件下侧向压力分布强度波动性定量描述中Ri与Ni拟合函数关系;Fig. 6 is the fitting function relationship between Ri and Ni in the quantitative description of the fluctuation of lateral pressure distribution intensity under the conditions of different particle sizes and particle friction coefficients;

图7—图11是不同颗粒粒径和颗粒摩擦系数条件下侧向压力分布图。Figures 7 to 11 are the lateral pressure distribution diagrams under the conditions of different particle sizes and particle friction coefficients.

具体实施方式Detailed ways

下面通过附图和实施例,对本发明的技术方案作进一步的具体说明。本实施例首先采用DEM数值模拟颗粒材料自然沉积过程,模拟参数参照DEM模拟石块、土体等颗粒材料相关文献选取[1,2],以确保模拟结果的正确性,模拟参数如表1所示。DEM数值模拟堆积稳定后的颗粒材料如图3所示,然后提取颗粒材料作用于左侧墙体的侧向压力,如图4(a)所示(颗粒粒径s为0.01m、颗粒摩擦μ系数为0.30)。采用本发明提供的一种颗粒材料侧向压力分布特征定量描述方法对图4(b)~(e)侧向压力进行定量描述。当作用于挡墙某些部位的侧向压力密集(应力集中),侧向压力强度骤增骤减时,挡墙在突变的力学边界条件下较易失稳。因此,本发明选取侧向压力作用位置密集度和分布强度波动性两个参数对侧向压力分布特征进行定量描述。本发明具体包括以下步骤:The technical solutions of the present invention will be further described in detail below through the accompanying drawings and embodiments. In this example, DEM is used to numerically simulate the natural deposition process of granular materials, and the simulation parameters are selected according to the literature related to DEM simulation of granular materials such as stones and soils [1, 2] to ensure the correctness of the simulation results. The simulation parameters are shown in Table 1. Show. The granular material after DEM numerical simulation is shown in Figure 3, and then the lateral pressure of the granular material acting on the left wall is extracted, as shown in Figure 4(a) (the particle size s is 0.01 m, the particle friction μ The coefficient is 0.30). A quantitative description method for lateral pressure distribution characteristics of granular materials provided by the present invention is used to quantitatively describe the lateral pressures in Figs. 4(b)-(e). When the lateral pressure applied to some parts of the retaining wall is dense (stress concentration) and the lateral pressure intensity increases and decreases suddenly, the retaining wall is more prone to instability under the sudden change of mechanical boundary conditions. Therefore, the present invention selects two parameters, the concentration of the action position of the lateral pressure and the fluctuation of the distribution intensity, to quantitatively describe the distribution characteristics of the lateral pressure. The present invention specifically includes the following steps:

步骤1,定义颗粒材料侧向压力分布位置密集度测量尺度。测量确定颗粒材料稳定堆积后的高度H0(单位为m),因为颗粒材料必须依靠挡墙才能稳定堆积,所以本领域也通常称之以挡墙高度H0,如图1所示。其中,线条1(纵向直线)表示挡墙,线条2(横向实线)表示侧向压力作用位置,线条3(横向虚线)表示等间距区间的分界线。根据分形理论[4],对于某个具有特定几何特征的事物,采用不同尺度ri对其几何特征进行度量得到相应的度量数目ni;当ri与ni之间具有

Figure BSA0000210039260000051
良好相关性时,可通过函数拟合得到ni=c1ri -d+c2,式中分布位置密集度测量尺度ri的单位为m,度量数目ni的单位为无量纲,c1和c2均为拟合得到的常数,单位均为无量纲,参数d为反映几何特征的常数,单位为无量纲。Step 1: Define the measurement scale of the location concentration of the lateral pressure distribution of the granular material. The measurement determines the height H 0 (unit is m) of the granular material after stable accumulation. Because the granular material must rely on the retaining wall to stably accumulate, it is also commonly referred to as the retaining wall height H 0 in the art, as shown in FIG. 1 . Among them, line 1 (longitudinal straight line) represents the retaining wall, line 2 (horizontal solid line) represents the action position of lateral pressure, and line 3 (horizontal dashed line) represents the dividing line of the equally spaced interval. According to the fractal theory [4] , for a thing with specific geometric characteristics, different scales ri are used to measure its geometric characteristics to obtain the corresponding measurement number ni ; when there is a difference between ri and ni
Figure BSA0000210039260000051
When the correlation is good, n i =c 1 r i -d +c 2 can be obtained by function fitting, where the unit of measurement scale ri of distribution location density is m, the unit of measurement number ni is dimensionless, c 1 and c 2 are constants obtained by fitting, and the unit is dimensionless. The parameter d is a constant reflecting geometrical characteristics, and the unit is dimensionless.

本实施方式中,颗粒材料稳定堆积后的高度H0为1.95m。在满足

Figure BSA0000210039260000052
条件下,选取一系列尺度参数r1=0.025m、 r2=0.030m、r3=0.035m、r4=0.040m。In this embodiment, the height H 0 after stable accumulation of the particulate material is 1.95 m. in satisfying
Figure BSA0000210039260000052
Under the conditions, a series of scale parameters r 1 =0.025m, r 2 =0.030m, r 3 =0.035m, and r 4 =0.040m were selected.

步骤2,获取不同测量尺度下侧向压力分布位置密集度的测量数目。测量尺度ri将挡墙平均划分成数目为

Figure BSA0000210039260000061
(若
Figure BSA0000210039260000062
为分数,则四舍五入为整数)、间距长度为ri的子组(相邻线条3之间)。统计子组中含有侧向压力作用点(线条2) 的子组数目ni(ni为整数)。Step 2: Obtain the measurement number of the density of lateral pressure distribution positions under different measurement scales. The measurement scale ri divides the retaining wall into a number of
Figure BSA0000210039260000061
(like
Figure BSA0000210039260000062
is a fraction, rounded to an integer), with a subgroup of interval length ri (between adjacent lines 3). Count the number of subgroups n i (n i is an integer) in the subgroup containing the lateral pressure application point (line 2).

本实施方式中,对于r1=0.025m,将挡墙平均划分成数目为78、间距长度为0.025m的子组,统计子组中包含侧向压力作用点的子组数目n1为63;对于 r2=0.030m,将挡墙平均划分成数目为65、间距长度为0.030m的子组,统计子组中包含侧向压力作用点的子组数目n2为54;对于r3=0.035m,将挡墙平均划分成数目为56、间距长度为0.035m的子组,统计子组中包含侧向压力作用点的子组数目n3为49;对于r4=0.040m,将挡墙平均划分成数目为49、间距长度为0.040m的子组,统计子组中包含侧向压力作用点的子组数目n4为46。In this embodiment, for r 1 =0.025m, the retaining walls are evenly divided into 78 subgroups with a spacing length of 0.025m, and the number of subgroups n 1 including lateral pressure action points in the statistical subgroups is 63; For r 2 =0.030m, the retaining walls are divided into 65 subgroups with a spacing length of 0.030m, and the number of subgroups n 2 including lateral pressure action points in the statistical subgroups is 54; for r 3 =0.035 m, the retaining wall is divided into 56 subgroups with a spacing length of 0.035m, and the number of subgroups n 3 including lateral pressure action points in the statistical subgroup is 49; for r 4 =0.040m, the retaining wall is divided into It is divided into 49 subgroups on average and the spacing length is 0.040m, and the number of subgroups n 4 including lateral pressure action points in the statistical subgroups is 46.

步骤3,求取描述侧向压力分布位置密集度参数d。将步骤2得到一系列(至少4组)ri和相应的ni绘制于双对数坐标系中,拟合logri与logni之间的线性关系,得到其可决系数R2(R2为无量纲,其越接近1,表明

Figure BSA0000210039260000063
相关性越强)。当R2大于0.8时,认为
Figure BSA0000210039260000064
存在较强的相关性,此时拟合直线斜率的绝对值即侧向压力分布位置密集度参数d。Step 3: Obtain a parameter d describing the location density of the lateral pressure distribution. Draw a series (at least 4 groups) ri and corresponding ni obtained in step 2 in the double logarithmic coordinate system, fit the linear relationship between logri and logni , and obtain the coefficient of determination R 2 (R 2 is dimensionless, the closer it is to 1, the more
Figure BSA0000210039260000063
the stronger the correlation). When R2 is greater than 0.8, it is considered that
Figure BSA0000210039260000064
There is a strong correlation. At this time, the absolute value of the slope of the fitting line is the density parameter d of the lateral pressure distribution position.

颗粒材料侧向压力分布位置密集度参数d为0~1之间数值,0表示作用位置分布几乎集中在某一点处,1则表示作用位置分布为线性连续分布。d越大,表明颗粒材料侧向压力分布位置越分散。The position density parameter d of the lateral pressure distribution of granular materials is a value between 0 and 1. 0 means that the action position distribution is almost concentrated at a certain point, and 1 means that the action position distribution is a linear continuous distribution. The larger the d is, the more dispersed the lateral pressure distribution position of the particulate material is.

本实施方式中,将步骤2得到r1=0.025m、r2=0.030m、r3=0.035m、 r4=0.040m和相应的n1=63、n2=54、n3=49、n4=46绘制于双对数坐标系中(图5所示),拟合logri(i=1,2,3,4)与logni(i=1,2,3,4)之间的线性函数关系,得到R2=0.98,表明

Figure BSA0000210039260000071
相关性强,拟合直线的斜率的绝对值即为参数 d=0.67。In this embodiment, r 1 =0.025m, r 2 =0.030m, r 3 =0.035m, r 4 =0.040m and corresponding n 1 =63,n 2 =54,n 3 =49, n 4 =46 is plotted in a double logarithmic coordinate system (shown in Figure 5), fitting between logr i (i=1, 2, 3, 4) and logn i (i=1, 2, 3, 4) The linear function relationship of , obtains R 2 =0.98, indicating that
Figure BSA0000210039260000071
The correlation is strong, and the absolute value of the slope of the fitted straight line is the parameter d=0.67.

步骤4,选取颗粒材料侧向压力分布强度波动性测量尺度。根据DEM数值模拟计算结果,以挡墙高度为纵轴,以颗粒材料的侧向压力为横轴,绘制颗粒材料侧向压力分布图。如图2所示,颗粒材料侧向压力沿挡墙高度的分布线是一条折线状的曲线,定义侧向压力分布折线的上、下两个端点分别为Pup和Pdown,如图2所示。选取一系列尺度参数Ri(i=1,2,…n),其中Ri满足

Figure BSA0000210039260000072
的条件。Step 4, select the measurement scale of the lateral pressure distribution intensity fluctuation of the granular material. According to the calculation results of DEM numerical simulation, take the height of the retaining wall as the vertical axis, and take the lateral pressure of the granular material as the horizontal axis, draw the lateral pressure distribution map of the granular material. As shown in Figure 2, the distribution line of the lateral pressure of granular materials along the height of the retaining wall is a polyline-like curve, and the upper and lower endpoints of the lateral pressure distribution polyline are defined as P up and P down , respectively, as shown in Figure 2. Show. Choose a series of scale parameters R i (i=1, 2,...n), where R i satisfies
Figure BSA0000210039260000072
conditions of.

本实施方式中,在满足

Figure BSA0000210039260000073
条件下,选取一系列尺度参数R1=0.1m、 R2=0.2m、R3=0.3m、R4=0.4m。定义侧向压力折线分布上、下两个端点分别为Pup和Pdown,如图4所示。In this embodiment, satisfying the
Figure BSA0000210039260000073
Under the conditions, a series of scale parameters R 1 =0.1m, R 2 =0.2m, R 3 =0.3m, R 4 =0.4m are selected. The upper and lower endpoints of the lateral pressure polyline distribution are defined as P up and P down , respectively, as shown in Fig. 4 .

步骤5,获取不同测量尺度下侧向压力分布强度波动性的测量数目。对于 R1=0.1m,以图4中颗粒材料侧向压力分布折线上端点Pup为圆心,以R1=0.1m 为半径画圆,圆与侧向压力分布折线相交于点P1;随后,以点P1为圆心,以 R1=0.1m为半径画圆,与侧向压力分布折线相交于点P2;以此类推,当交点P139与Pdown在侧向压力折线距离l=0.011小于R1=0.1m时,测量结束,最终得到以 R1=0.1m为尺度量取侧向压力分布折线的数目 N1=n+l/R1=139+0.011/0.1=139.11,如图4(b)所示。采用上述相同的方法可得N2=60.12、N3=30.05、N4=26.78。Step 5: Obtain the measurement number of the intensity fluctuation of the lateral pressure distribution under different measurement scales. For R 1 =0.1m, take the endpoint P up on the lateral pressure distribution line of the granular material in Fig. 4 as the center of the circle, and draw a circle with R 1 =0.1m as the radius. The circle intersects the lateral pressure distribution line at point P 1 ; then , draw a circle with point P 1 as the center and R 1 =0.1m as the radius, and intersect with the lateral pressure distribution line at point P 2 ; and so on, when the intersection point P 139 and P down are at a distance l= When 0.011 is less than R 1 =0.1m, the measurement ends, and finally the number of broken lines of lateral pressure distribution measured with R 1 =0.1m as the scale N 1 =n+l/R 1 =139+0.011/0.1=139.11 is obtained, such as shown in Figure 4(b). Using the same method as above, N 2 =60.12, N 3 =30.05, and N 4 =26.78 can be obtained.

步骤6,求取描述侧向压力分布强度波动性参数。将步骤5得到R1=0.1m、 R2=0.2m、R3=0.3m、R4=0.4m和相应的N1=139.11、N2=60.12、N3=30.05、N4=26.78绘制于双对数坐标系中(图6所示)。拟合logRi(i=1,2,3,4)与 logNi(i=1,2,3,4)之间的线性函数关系,得到R2=0.95,表明

Figure BSA0000210039260000081
相关性强(R2越接近1,表明
Figure BSA0000210039260000082
相关性越强),拟合直线的斜率的绝对值即为侧向压力分布强度波动性参数D=1.23。Step 6: Obtain parameters describing the fluctuation of lateral pressure distribution intensity. Plot the steps 5 for R1 = 0.1m, R2=0.2m, R3 =0.3m, R4=0.4m and corresponding N1 = 139.11 , N2 =60.12, N3 = 30.05, N4 =26.78 in a double logarithmic coordinate system (shown in Figure 6). Fitting the linear functional relationship between logR i (i=1, 2, 3, 4) and logN i (i=1, 2, 3, 4), R 2 =0.95 is obtained, indicating that
Figure BSA0000210039260000081
Strong correlation (the closer R is to 1 , the more
Figure BSA0000210039260000082
The stronger the correlation), the absolute value of the slope of the fitted straight line is the lateral pressure distribution intensity fluctuation parameter D=1.23.

颗粒材料侧向压力分布强度波动性参数D值在1~2之间,1表示侧向压力强度分布为直线分布,2则表示侧向压力强度分布为平面分布。D越大表明侧向压力分布强度波动性越大,拱结构效应越明显,侧向压力骤增点越多。The value of the fluctuation parameter D of the lateral pressure distribution intensity of granular materials is between 1 and 2. 1 means that the lateral pressure intensity distribution is a linear distribution, and 2 means that the lateral pressure intensity distribution is a plane distribution. The larger the D, the greater the fluctuation of the lateral pressure distribution intensity, the more obvious the arch structure effect, and the more the lateral pressure sudden increase points.

此外,在保证其他数值计算参数不变的条件下,通过改变颗粒粒径s(土为 0.01m、石为0.40m)和颗粒摩擦系数μ(0.30、0.60、0.90)以得到不同条件下颗粒材料侧向压力分布,如图7-图11所示;利用本发明的技术方案分别对其分布位置密集度和分布强度波动性进行定量描述,以验证本发明技术方案的适用性。In addition, under the condition of keeping other numerical calculation parameters unchanged, by changing the particle size s (0.01m for soil, 0.40m for stone) and particle friction coefficient μ (0.30, 0.60, 0.90) to obtain granular materials under different conditions The lateral pressure distribution is shown in Fig. 7-Fig. 11; using the technical solution of the present invention to quantitatively describe its distribution location density and distribution intensity fluctuation, respectively, to verify the applicability of the technical solution of the present invention.

表2给出了采用本发明技术方案计算得到的不同颗粒粒径和颗粒摩擦系数条件下颗粒材料侧向压力分布位置尺度参数ri、相应数目ni、密集度定量描述参数d以及侧向压力分布强度尺度参数Ri、相应数目Ni、分布强度波动性定量描述参数D。不同颗粒粒径和颗粒摩擦系数条件下ri与ni、Ri与Ni拟合函数分别如图5和图6所示。Table 2 shows the position scale parameter r i , the corresponding number ni , the quantitative description parameter d of the density and the lateral pressure of the granular material under the conditions of different particle sizes and particle friction coefficients calculated by the technical solution of the present invention The distribution intensity scale parameter R i , the corresponding number N i , the distribution intensity volatility quantitative description parameter D. The fitting functions of ri and ni and Ri and Ni under different particle size and particle friction coefficient are shown in Fig. 5 and Fig. 6 , respectively.

可以看出,不同条件下ni

Figure BSA0000210039260000083
Ni
Figure BSA0000210039260000084
均有很强的相关性。因此本发明能够客观有效地定量描述颗粒材料侧向压力分布特征。颗粒材料侧向压力分布位置密集度描述参数d受颗粒粒径和颗粒摩擦系数影响较大;颗粒粒径和颗粒摩擦系数越大,则d越小,表明侧向压力分布位置越密集,越不利于刚性挡墙的安全稳定。颗粒材料侧向压力分布强度波动性描述参数D受颗粒粒径和颗粒摩擦系数影响不大,分布范围在1.17~1.29之间。It can be seen that under different conditions, n i and
Figure BSA0000210039260000083
Ni and
Figure BSA0000210039260000084
are strongly correlated. Therefore, the present invention can objectively and effectively quantitatively describe the lateral pressure distribution characteristics of granular materials. The density description parameter d of the lateral pressure distribution of granular materials is greatly affected by the particle size and the particle friction coefficient; the larger the particle size and the particle friction coefficient, the smaller the d, indicating that the lateral pressure distribution is denser and less stable. Conducive to the safety and stability of rigid retaining walls. The description parameter D of the lateral pressure distribution intensity fluctuation of granular material is not greatly affected by particle size and particle friction coefficient, and the distribution range is between 1.17 and 1.29.

目前工程实践和物理试验难以全面获取堆积稳定后的颗粒材料的侧向压力分布,而离散单元法DEM数值模拟则可精细化得到颗粒材料侧向压力分布信息。本发明方法主要应用于定量描述离散单元法DEM数值模拟得到的颗粒材料侧向压力分布位置密集度和分布强度波动性,有助于从细观层面上指导挡墙、基坑等工程设计。本发明方法以分形理论的思想为理论基础,进一步明确针对描述颗粒材料侧向压力特征的测量尺寸取值范围,描述参数简单有效,物理意义明确,适用性强,能够真实反映出颗粒材料侧向压力分布的离散特征。At present, it is difficult to fully obtain the lateral pressure distribution of granular materials after stable accumulation in engineering practice and physical tests. However, the discrete element method DEM numerical simulation can refine the lateral pressure distribution information of granular materials. The method of the invention is mainly applied to quantitatively describe the lateral pressure distribution position density and distribution intensity fluctuation of granular materials obtained by the discrete element method DEM numerical simulation, and is helpful for guiding engineering design of retaining walls and foundation pits from a mesoscopic level. The method of the invention is based on the idea of fractal theory, further clarifies the range of the measurement size for describing the lateral pressure characteristics of the granular material, the description parameters are simple and effective, the physical meaning is clear, the applicability is strong, and the lateral pressure of the granular material can be truly reflected. Discrete features of the pressure distribution.

表1 DEM数值模拟计算参数Table 1 DEM numerical simulation calculation parameters

Figure BSA0000210039260000091
Figure BSA0000210039260000091

表2 不同颗粒粒径s、颗粒摩擦系数μ下侧向压力分布位置密集度定量描述Table 2 Quantitative description of the location density of lateral pressure distribution under different particle size s and particle friction coefficient μ

Figure BSA0000210039260000101
Figure BSA0000210039260000101

表3 不同颗粒粒径s、颗粒摩擦系数μ下侧向压力分布强度波动性定量描述Table 3 Quantitative description of lateral pressure distribution intensity fluctuation under different particle size s and particle friction coefficient μ

Figure BSA0000210039260000102
Figure BSA0000210039260000102

Claims (1)

1. A quantitative description method for the lateral pressure distribution characteristics of a granular material is characterized by comprising the following steps:
step 1, selecting a particle material lateral pressure distribution position concentration measurement scale: measuring the height H after the particulate material has been settled0(also referred to as wall height in m) by selecting a series of measurement scale parameters ri(i ═ 1, 2, … n), where riSatisfy the requirement of
Figure FSA0000210039250000011
The conditions of (1).
Step 2, obtaining the measurement number of the lateral pressure distribution position concentration under different measurement scales: measurement scale riDividing the retaining wall into equal number
Figure FSA0000210039250000012
A pitch length of riThe statistical subgroup contains the subgroup number n of lateral pressure action pointsi
Step 3, solving a parameter d for describing the lateral pressure distribution position concentration: a series of r obtained in step 2iAnd corresponding niDrawing in a log-log coordinate system, and fitting log riAnd log niLinear relation between them, and obtaining its coefficient of determination R2When R is2And when the absolute value of the slope of the fitting straight line is more than 0.8, the absolute value of the slope of the fitting straight line is the lateral pressure distribution position concentration parameter d.
The lateral pressure distribution position concentration parameter d of the granular material is a numerical value between 0 and 1, wherein 0 represents that the action position distribution is almost concentrated at a certain point, and 1 represents that the action position distribution is linearly and continuously distributed. A larger d indicates a more dispersed location of the pressure distribution laterally of the particulate material.
Step 4, selecting a particle material lateral pressure distribution intensity fluctuation measurement scale: drawing a lateral pressure distribution diagram of the granular material, and defining the upper end point and the lower end point of a lateral pressure broken line as P respectivelyupAnd PdownSelecting a series of scale parameters Ri(i ═ 1, 2, … n), where R isiSatisfy the requirement of
Figure FSA0000210039250000013
The conditions of (1).
Step 5, obtaining the measurement number of the lateral pressure distribution intensity fluctuation under different measurement scales: the upper end point P of the broken line is distributed by the lateral pressure of the granular materialupAs a circle center, with RiDrawing a circle for the radius, said circle intersecting the lateral pressure distribution polyline at a point P1(ii) a Then, again at point P1As a circle center, with RiIs a circle drawn by the radius and intersects the side pressure distribution broken line at a point P2(ii) a By analogy, when the intersection point PnAnd PdownThe distance l on the lateral pressure distribution broken line is less than or equal to RiWhen the measurement is finished, the final result is RiMeasuring the number N of lateral pressure distribution polylines for a scalei=n+l/Ri
And 6, solving the fluctuation parameters for describing the lateral pressure distribution strength. Subjecting step 5 to obtain a series of RiAnd corresponding NiDrawing in a log-log coordinate system, and fitting log RiAnd log NiLinear function relationship between them to obtain its coefficient of determinability R2(ii) a When fitting the coefficient of the function2And when the absolute value of the slope of the fitting straight line is more than 0.8, the absolute value of the slope of the fitting straight line is the lateral pressure distribution intensity fluctuation parameter D.
The value of the fluctuation parameter D of the lateral pressure distribution intensity of the particle material is between 1 and 2, wherein 1 represents that the lateral pressure intensity distribution is in a straight line distribution, and 2 represents that the lateral pressure intensity distribution is in a plane distribution. The larger D indicates the larger fluctuation of the lateral pressure distribution intensity, the more obvious arch structure effect is, and the more lateral pressure sudden increase points are.
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CN110334431A (en) * 2019-07-02 2019-10-15 西南石油大学 A method for single well controlled reserves calculation and residual gas analysis in low permeability tight gas reservoirs

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RU2010122384A (en) * 2010-06-01 2011-12-10 Сергей Иванович Малафеев (RU) METHOD FOR VISUALIZING EXTRUDER WORK
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CN109359416A (en) * 2018-11-07 2019-02-19 河北工业大学 A Particle Flow Numerical Simulation Method Reflecting the Distribution of Real Engineering Soil-rock Mixtures
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