Published in Advances in Computational Plasticity. Computational Methods in Applied Sciences. Oñate, E., Peric, D., de Souza Neto, E., Chiumenti, M., (Eds.), Vol. 46, pp. 309-335, Springer, 2018
DOI: /10.1007/978-3-319-60885-3_15

## Abstract

In this chapter we present recent advances in the Discrete Element Method (DEM) and in the coupling of the DEM with the Finite Element Method (FEM) for solving a variety of problems in non linear solid mechanics involving damage, plasticity and multifracture situations.

## 1. Introduction

The Discrete Element Method (DEM) is a popular technique for analysis of the mechanics of granular matter, as well as for modeling multifracture situations in frictional materials such as concrete and geomaterials.

The Finite Element Method (FEM), on the other hand, is a standard numerical technique for linear and non linear analysis of structures. Differently from the DEM, the FEM has difficulties for reproducing multifracture situations in solids. The combination of FEM and DEM procedures seems therefore a win-win situation for modeling and simulation of a wider range of problems in non linear mechanics, than using any of the two methods separately.

In this chapter we present first recent advances in the DEM for non linear analysis of cohesive and non cohesive materials. Then a method for coupling the DEM and FEM procedures and for studying the interaction of physical particles and deformable solids es explained. In the last part of the chapter we present an approach for modeling multifracture situations in a solid by starting with the FEM analysis of the continuum domain in the standard manner. Discrete elements at the element nodes are progressively introduced as damage on the center of the element sides exceeds a certain value. Examples of this FEM-DEM technique are presented for a number of structural problems involving single fracture and multifracture situations such as the failure analysis of concrete samples and beams under external loads, a shale rock domain under a pulse load and blasting situations in a tunnel front and a granite rock specimen.

## 2. A local DEM model

### 2.1 DEM model overview

The DEM was initially developed by Cundall et al. [5] in the 1970's. It is based in the interaction of discrete elements (also called particles) – typically cylinders (in 2D) and spheres (in 3D) – to simulate the behavior of continuum and discontinuum domains [2,3,6,7,12,14,15,21,24,26,31]. This interaction is governed by a set of kinematic equations involving the forces acting over the discrete elements and the displacements, velocities and accelerations of the particles. The forces acting over a discrete element are related to the stresses and strains according to a constitutive model. In our work we use the local constitutive model for the DEM for cohesive and non-cohesive materials proposed by Oñate et al. [21]. In the following a brief description of this model is presented.

 Figure 1: Motion of a rigid particle
 (a) (b) Figure 2: (a) Definition of contact interface between two discrete particles. (b) Forces acting along the normal and shear directions on a contact interface section ${\displaystyle A^{ij}}$

#### 2.1.1 Kinematic equations and integration scheme

The translation and rotation of the particles in the DEM is governed by the standard dynamics equations for rigid bodies,

 ${\displaystyle m_{i}{\ddot {\mathbf {u} }}_{i}={\mathbf {F} }_{i}\qquad ,\qquad {\mathbf {I} }_{i}{\dot {\mathbf {\omega } }}_{i}={\mathbf {T} }_{i}}$
(1)

where ${\textstyle {u}_{i}}$ and ${\textstyle {\mathbf {\omega } }_{i}}$ are the ${\textstyle i}$-th particle displacement and the angular velocity respectively, ${\textstyle m_{i}}$ and ${\textstyle {I}_{i}}$ are the mass and the inertia tensor of the particle, and ${\textstyle {F}_{i}}$ and ${\textstyle {T}_{i}}$ are vectors containing the forces and torques due to the interaction of a particle with its neighbors (Figure 1). The set of forces applied on a particle include external forces (${\textstyle {\mathbf {F} }_{i}^{ext}}$), damping forces (${\textstyle {\mathbf {F} }_{i}^{damp}}$) and interaction forces between neighbor particles (${\textstyle {\mathbf {F} }^{ij}}$) (Figure 2)

 ${\displaystyle {\mathbf {F} }_{i}={\mathbf {F} }_{i}^{ext}+{\mathbf {F} }_{i}^{damp}+\sum \limits _{j=1}^{n_{i}}{\mathbf {F} }^{ij}}$
(2)

where ${\textstyle n}$ is the number of particles adjacent to the ${\textstyle i}$th particle.

The expression for the torques can be derived from Eq.(2) [22]. The dynamic equations (1) are integrated in time using an explicit scheme as expressed in (3) for the translation motion,

 ${\displaystyle {\ddot {\mathbf {u} }}_{i}^{n}={\frac {{\mathbf {F} }_{i}^{n}}{m_{i}}}\quad ,\quad {\dot {\mathbf {u} }}_{i}^{n+1/2}={\dot {\mathbf {u} }}_{i}^{n-1/2}+{\ddot {\mathbf {u} }}_{i}^{n}\Delta t\quad ,\quad {\mathbf {u} }_{i}^{n+1}={\mathbf {u} }_{i}^{n}+{\dot {\mathbf {u} }}_{i}^{n+1/2}\Delta t}$
(3)

The explicit time integration scheme is chosen due to the high computational cost of the DEM solution for large problems. However, the stability of the scheme is conditioned to the time step value. The critical time step is related to the high frequency of the problem, (${\textstyle \omega ^{max}}$), i.e.

 ${\displaystyle \Delta t\leq {\Delta t}_{cr}={\frac {2}{\omega ^{max}}}\left({\sqrt {1+\xi ^{2}}}-\xi \right)}$
(4)

where ${\textstyle \xi }$ is a fraction of the critical damping [5,22].

#### 2.1.2 Forces acting over the discrete element

The interaction forces at the contact interface between two particles i and j (${\textstyle {F}^{ij}}$) are obtained from the normal (${\textstyle {F}_{n}^{ij}}$) and tangential (${\textstyle {F}_{s}^{ij}}$) components (Figure 2b).

The normal component of the interaction forces is calculated as,

 ${\displaystyle {F}_{n}^{ij}=\sigma _{n}\alpha _{ij}{A}^{ij}\quad {\hbox{with }}{A}^{ij}=\pi r_{c}^{2}}$
(5)

where ${\textstyle \sigma _{n}}$ is the normal stress at the contact interface, ${\textstyle r_{c}}$ is the minimum radius of the two interacting particles (Figure 2a) and ${\textstyle \alpha _{ij}}$ is a parameter that dependes on the number of contacts and the packing of the particles [21]. In our work we have used a global definition of ${\textstyle \alpha _{ij}=\alpha =40{\frac {P}{N_{c}}}}$ where ${\textstyle N_{c}}$ and ${\textstyle P}$ are respectively the average number of contacts per sphere and the average porosity for the whole particle assembly [21]. The normal stress ${\textstyle \sigma _{n}}$ is calculated from the strain ${\textstyle \xi _{n}}$ and the strain rate ${\textstyle {\dot {\xi }}_{n}}$ along the normal direction as,

 ${\displaystyle \sigma _{n}=E\varepsilon _{n}+c{\dot {\varepsilon }}_{n}}$
(6)

where ${\textstyle E}$ is the Young modulus, ${\textstyle c}$ is a local damping parameter calculated as

 ${\displaystyle c=2{\frac {\xi }{r_{c}}}{\sqrt {m_{ij}K_{n}^{ij}}}\quad {\hbox{with}}\quad m_{ij}={\frac {m_{i}m_{j}}{m_{i}+m_{j}}}}$
(7)

where ${\textstyle K_{n}^{ij}}$ is the normal stiffness parameter (see Eq.(10)).

The normal strain and strain rate values are computed from the kinematic variables as,

 ${\displaystyle \varepsilon _{n}={\frac {u_{n}}{d_{ij}}}\qquad {\dot {\varepsilon }}_{n}={\frac {{\dot {u}}_{n}}{d_{ij}}}}$
(8)

where ${\textstyle u_{n}}$ and ${\textstyle {\dot {u}}_{n}}$ are the relative displacements and the relative velocity between two particles along the normal direction at the contact interface and ${\textstyle d_{ij}}$ is the distance between the centroids of the two particles (Figure 2b).

Equations (5)–(8) lead to a general relation between for the normal force and the kinematic variables as

 ${\displaystyle {F}_{n}^{ij}={\frac {\alpha _{ij}{A}^{ij}}{d_{ij}}}\left[Eu_{n}+2{\frac {\xi }{r_{c}}}{\sqrt {m_{ij}K_{n}}}{\dot {u}}_{n}\right]=K_{n}^{ij}u_{n}+C_{n}^{ij}{\dot {u}}_{n}}$
(9)

where ${\textstyle K_{n}^{ij}}$ and ${\textstyle C_{n}^{ij}}$ are the normal stiffness and the normal viscous damping parameters at the contact interface between particles ${\textstyle i}$ and ${\textstyle j}$ that can be deduced from Eq.(9) as

 ${\displaystyle K_{n}^{ij}={\frac {\alpha _{ij}{A}^{ij}}{d_{ij}}}E\quad ,\quad C_{n}^{ij}={\frac {2\alpha _{ij}{A}^{ij}\xi }{d_{ij}r_{c}}}{\sqrt {m_{ij}K_{n}}}}$
(10)

A similar approach leads to the constitutive expression for the shear forces in the two tangential directions as [21]

 ${\displaystyle {\mathbf {F} }_{s}^{ij}=K_{s}^{ij}{\mathbf {u} }_{s}^{ij}}$
(11)

where vector ${\textstyle {\mathbf {u} }_{s}^{ij}}$ is the shear component of the relative displacements between particles, calculated as,

 ${\displaystyle {\mathbf {u} }_{s}^{ij}={\mathbf {u} }^{ij}-\left({\mathbf {u} }^{ij}{\mathbf {n} }^{ij}\right){\mathbf {n} }^{ij}}$
(12)

In Eq.(11) ${\textstyle K_{s}^{ij}}$ is the shear stiffness parameter at the contact interface (assumed to be the same for both shear directions), given by

 ${\displaystyle K_{s}^{ij}={\frac {K_{n}^{ij}}{2\left(1+\nu \right)}}}$
(13)

where ${\textstyle \nu }$ is the Poisson's ratio of the material.

The damping forces are computed from the application of a global damping over the set of particles. This damping component is characterized by translation (${\textstyle \alpha ^{t}}$) and rotation (${\textstyle \alpha ^{r}}$) damping parameters defined as a fraction of the stiffness parameters. In this work we have taken ${\textstyle \alpha ^{r}=\alpha ^{t}=0,10}$. The damping forces act in opposite direction to the motion of the particles according to the following expressions:

 ${\displaystyle {\mathbf {F} }_{i}^{damp}=-\alpha ^{t}\left|{\mathbf {F} }_{i}^{ext}+{\mathbf {F} }^{ij}\right|{\frac {{\dot {\mathbf {u} }}_{i}}{\left|{\dot {\mathbf {u} }}_{i}\right|}}}$
(14.a)

 ${\displaystyle {\mathbf {T} }_{i}^{damp}=-\alpha ^{r}\left|{\mathbf {T} }_{i}\right|{\frac {{\dot {\mathbf {\omega } }}_{i}}{\left|{\dot {\omega }}_{i}\right|}}}$
(14.b)

The local DEM constitutive model described above holds for cohesive and non-cohesive materials, this latter as a particular case of the former, when the bonds between the particles are assumed to be initially broken. More details can be found in [21].

### 2.2 Normal and shear failure

Cohesive bonds at a contact interface are assumed to start breaking when the interface strength is exceeded in the normal direction by the tensile contact force, or in the tangential direction by the shear force. The uncoupled failure (decohesion) criterion for the normal and tangential directions at the contact interface between particles ${\textstyle i}$ and ${\textstyle j}$ is written as

 ${\displaystyle F_{n_{t}}\geq {\cal {F}}_{n_{t}}\quad ,\quad F_{s}\geq {\cal {F}}_{s}}$
(15)

where ${\textstyle {\cal {F}}_{n_{t}}}$ and ${\textstyle {\cal {F}}_{s}}$ are the interface strengths for pure tension and shear-compression conditions, respectively, ${\textstyle F_{n_{t}}}$ is the normal tensile force and ${\textstyle {F}_{s}}$ is the modulus of the shear force vector ${\textstyle {F}_{s}^{ij}}$ (Figure 2 and Eq.(11)).

The interface strengths are defined as

 ${\displaystyle {\cal {F}}_{n_{t}}=\sigma _{t}^{f}{\bar {A}}^{ij}\quad ,\quad {\cal {F}}_{s}=\tau ^{f}{\bar {A}}^{ij}+\mu _{1}\vert F_{n_{c}}\vert }$
(16)

where ${\textstyle \sigma _{t}^{f}}$ and ${\textstyle \tau ^{f}}$ are the tensile and shear strengths respectively, ${\textstyle F_{n_{c}}}$ is the compressive normal force at the contact interface and ${\textstyle \mu _{1}=\tan \phi _{1}}$ is a (static) friction parameter, where ${\textstyle \phi _{1}}$ is an internal friction angle. These values are assumed to be an intrinsic property of the material and are determined experimentally. In our work ${\textstyle \sigma _{t}^{f}}$ is taken as the tensile strength of the material measured in a bending-tensile (BT) or a Brasilian tensile strength test [21].

As for the shear strength ${\textstyle \tau ^{f}}$ we have estimated its value as a percentage of the maximum compressive stress in a uniaxial compression strength (UCS) test, ${\textstyle (\sigma _{n_{c}}^{f})_{UCS}}$, as

 ${\displaystyle \tau ^{f}=\beta (\sigma _{n_{c}}^{f})_{UCS}}$
(17)

where ${\textstyle \beta }$ is a parameter that is calibrated in numerical experiments via shear and UCS tests. Typically ${\textstyle \beta \simeq 0.5}$ [21].

Following tension failure, the constitutive behavior in the shear direction is governed by the standard Coulomb law

 ${\displaystyle {F}_{s}=\mu _{2}\vert F_{n_{c}}\vert {\frac {{u}_{s}}{|{u}_{s}|}}\quad {\hbox{with}}\quad \mu _{2}=\tan \phi _{2}}$
(18)

where ${\textstyle \mu _{2}}$ is a dynamic Coulomb friction coefficient and ${\textstyle \phi _{2}}$ is the post-failure internal friction angle. Both parameters are determined from experimental tests.

Figure 3 shows the graphical representation of the failure criterium described by Eqs.(15), (16) and (18). This criterium assumes that the tension and shear forces contribute to the failure of the contact interface in a decoupled manner. On the other hand, shear failure under normal compressive forces follows a failure line that is a function of the shear failure stress, the compression force and the internal friction angle.

Indeed, a coupled failure model in the tension-shear zone can also be used, as described in [21]. For the numerical tests presented in this work the uncoupled model has been used.

Figure 4 shows the evolution of the normal tension force ${\textstyle F_{n_{t}}}$ and the shear force modulus ${\textstyle F_{s}}$ at a contact interface until failure in terms of the relative normal and tangential displacement increments. Elastic damage under tensile and shear conditions has been taken into account in this work by assuming a linear softening behaviour defined by the softening moduli ${\textstyle H_{n}}$ and ${\textstyle H_{t}}$ introduced into the force-displacement relationships in the normal (tensile) and shear directions, respectively (Figure 4). For details see [21].

 Figure 3. Failure line in terms of normal and shear forces. Uncoupled failure model. (b) Coupled failure model
 Figure 4. Undamaged and damaged elastic moduli under tension (a) and shear (b) forces

### 2.3 Elasto-plastic model for compression forces

The compressive stress-strain behaviour in the normal direction at the contact interface for frictional cohesive materials, such as cement, rock and concrete, is typically governed by an initial elastic law followed by a non-linear constitutive equation that varies for each material. The compressive normal stress increases under linear elastic conditions until it reaches the limit normal compressive stress ${\textstyle \sigma _{n_{c}}^{l}}$. This is defined as the axial stress level where the experimental curve relating the axial stress and the axial strain starts to deviate from the linear elastic behaviour. After this point the material is assumed to yield under elastic-plastic conditions.

The elasto-plastic relationships in the normal compressive direction are defined as

 ${\displaystyle dF_{n_{c}}=K_{T_{n}}du_{n}}$
(19.a)

 ${\displaystyle dF_{n_{c}}=K_{n_{0}}du_{n}}$
(19.b)

In Eqs.(3.3) ${\textstyle dF_{n_{c}}}$ and ${\textstyle du_{n}}$ are respectively the variation of the normal compressive force and the normal (relative) displacement, ${\textstyle K_{n_{0}}}$ is the initial (elastic) compressive stiffness for a value of ${\textstyle E=E_{0}}$ (Figure 5), and ${\textstyle K_{T_{n}}}$ is the tangent compressive stiffness given by

 ${\displaystyle K_{T_{n}}={\frac {E_{T}}{E_{0}}}K_{n_{0}}}$
(20)

where ${\textstyle E_{T}}$ is the slope of the normal stress-strain curve in the elastoplastic branch (i.e. ${\textstyle E_{T}=E_{1}}$, ${\textstyle E_{2}}$, ${\textstyle E_{3}}$ in Figure 5).

Plasticity effects in the normal compressive direction affect the evolution of the tangential forces at the interface, as the interface shear strength is related to the normal compression force by Eq.(16).

Figure 5 shows the diagram relating the compressive axial stress and the compressive axial strain used for modelling the elasto-plastic constitutive behaviour at the contact interfaces. The form of each diagram is obtained from experimental tests [8].

 Figure 5: Compressive axial stress-compressive axial strain diagram for elastoplastic material. LCS1 is the limit compressive stress (${\displaystyle \sigma _{n_{c}}^{l}}$) defining the onset of elastoplastic behaviour at the contact interface

Figures 6 and 7 show an example of the DEM to the analysis of application of a UCS test and a BST of a cylindrical specimen for a cement material. The material parameter are shown in Table 1.

Table 1. DEM constitutive parameters for analysis of UCS and BTS tests on a cement sample
 ${\textstyle \rho }$ ${\displaystyle \mu _{1}}$ ${\displaystyle \mu _{2}}$ ${\displaystyle E_{0}}$ ${\displaystyle \nu }$ ${\displaystyle \sigma _{t}^{f}}$ ${\displaystyle \tau _{f}}$ (g/cc) (GPa) (MPa) (MPa) 1.70 0.30 0.40 3.80 0.20 4.80 8.50 LCS1 LCS2 LCS3 YRC1 YRC2 YRC3 ${\displaystyle \alpha }$ (MPa) (MPa) (MPa) 8.5 9.0 11 3 9 24 1.0
 (a) (b) Figure 6: DEM and experimental results for UCS test in a cement sample using 42000 spherical particles. (a) Axial stress-axial strain curve. (b) Contour of the horizontal displacement at the failure load
 (a) (b) Figure 7: DEM results for BTS test in cement sample using 16000 spheres. (a) Time evolution of the stress at the center point. (b) Contour of horizontal displacement at the failure load. The experimental failure stress is 3MPa

### 2.4 Enhanced local constitutive model for the DEM that accurately reproduces the behavior of a continnum

The standard DEM technique is known to suffer from sensitivity to the packaging pattern and density of the particles when applied to the linear elastic analysis of a continuum. Standard features of a continuum domain, such as the Poisson's ratio effect, are difficult to predict with the DEM in a consistent manner.

Celigueta et al. [2] have presented a procedure for correcting the local constitutive equations at a contact interface in the DEM, so that it can be accurately applied for predicting the elastic behavior of a continuum.

The enhanced local constitutive model for the DEM is based on a modified expression of the force-displacement relationships at the contact interface between particles ${\textstyle i}$ and ${\textstyle j}$ (Eqs.9 and 11) as follows

 ${\displaystyle F_{n}^{ij}=K_{n}^{ij}u_{n}^{ij}+{\underline {A^{ij}\nu (\sigma _{s_{1}}^{ij}+\sigma _{s_{2}}^{ij})}}A^{ij}\nu (\sigma _{s_{1}}^{ij}+\sigma _{s_{2}}^{ij})}$ (21) ${\displaystyle F_{s_{k}}^{ij}=K_{s}^{ij}u_{s_{k}}^{ij}+{\underline {GA^{ij}\left({\frac {\partial u_{n}}{\partial s_{k}}}\right)^{ij}}}GA^{ij}\left({\frac {\partial u_{n}}{\partial s_{k}}}\right)^{ij}\quad ,\quad k=1,2}$ (22)

where ${\textstyle K_{n}^{ij}}$ and ${\textstyle K_{s}^{ij}}$ are the normal and tangential stiffness parameters associated to the contact interface given by Eqs.10 and 12, respectively and ${\textstyle u_{s_{k}}}$ is the relative displacement in the ${\textstyle k}$th tangential direction (Figure 2).

The underlined terms in Eqs.21 and 22 introduce the effect of the average stress field at the contact interface on the normal and tangential forces at the interface. Details of the computation of these terms is given in [2].

The stresses ${\textstyle \sigma _{s_{1}}}$ and ${\textstyle \sigma _{s_{2}}}$ in Eq.21 are obtained by projecting the average stress tensor ${\textstyle [\sigma ]^{i}}$ for the ${\textstyle i}$th particle into the local coordinate system (${\textstyle {s}_{1},{s}_{2},{n}}$) (Figure 2b). Tensor ${\textstyle [\sigma ]^{i}}$ is computed as

 ${\displaystyle [\sigma ]^{i}={\frac {1}{V_{i}}}\sum \limits _{i=1}^{n_{i}}{l}_{i}\otimes {F}_{i}}$
(23)

where ${\textstyle n_{i}}$ is the number of contact points for the ${\textstyle i}$th particle, ${\textstyle {l}_{i}}$ is the vector connecting the center of the particle to the ${\textstyle i}$th contact point, ${\textstyle {F}_{i}}$ is the force vector at the ${\textstyle i}$th contact point and ${\textstyle V_{i}}$ is a volume associated to the particle used to average the stresses.

A good estimation of ${\textstyle V_{i}}$ is essential for the success of this approach. In our work we have estimated ${\textstyle V_{i}}$ using the areas of the contact interfaces associated to each particle as

 ${\displaystyle V_{i}=\sum \limits _{j=1}^{n_{i}}{\frac {1}{3}}{\hat {A}}^{ij}\Vert {l}_{i}\Vert }$
(24)

where ${\textstyle {\hat {A}}^{ij}}$ is an enhanced value of the area of the contact interface between particles ${\textstyle i}$ and ${\textstyle j}$. The value of ${\textstyle {\hat {A}}^{ij}}$ is computed as

 ${\displaystyle {\hat {A}}^{ij}=A^{ij}{\frac {4\pi \alpha _{i}r_{i}^{2}}{A_{i}^{T}}}}$
(25)

where ${\textstyle A^{ij}}$ is the area of the ${\textstyle j}$th contact interface computed by Eq.5, ${\textstyle r_{i}}$ is the radius of the ${\textstyle i}$th particle, ${\textstyle A_{i}^{T}}$ is the sum of the contact interface areas ${\textstyle \left(A_{i}^{T}=\sum \limits _{j=1}^{n_{i}}A^{ij}\right)}$ and ${\textstyle \alpha _{i}}$ is a parameter that depends on the number of neighboring particles to the ${\textstyle i}$th particle and on the uniformity of the contact areas due to a random distribution of the particle sizes. More details are given in [2].

The non-local terms in Eqs.21 and 22 have proven to be essential for accurately predicting the elastic and non-linear response of samples of cohesive material using the DEM.

As an example Table 2 shows the expected and computed values for the Young's modulus and the Poissson's ratio for a prismatic sample of elastic material modelled with cartesian, staggered and random distribution of spheres. Note the large errors for the values of ${\textstyle E}$ and ${\textstyle \nu }$ using the standard DEM for staggered and random packings. The errors are negligible when the enhanced local constitutive model for the DEM presented in the previous lines is used.

The enhanced local constitutive model for the DEM has also shown an excellent behavior for accurately predicting the non-linear response and cracking pattern of geomaterials and concrete using a simple Rankine failure model at the contact interface.

Table 2. Prediction of ${\displaystyle E}$ and ${\displaystyle \nu }$ in a sample using the normal and tangential contact forces
 Input parameters: ${\displaystyle E=1.0e9}$, ${\displaystyle \nu =0.35}$ Cartesian packing Staggered packing Random packing Standard Improved Standard Improved Standard Improved DEM DEM DEM DEM DEM DEM Poisson's ratio ${\textstyle E}$ -0.6 % -0.6 % -23.0 % 0.7 % -28.0 % -0.2 Poisson's ratio ${\textstyle \nu }$ -100.0 % 0.22 % -64.0 % -2.9 % -62.0 % -3.5

We present an application of the enhanced local constitutive model for the DEM to the analysis of a shear test [16] in a cylindrical notched specimen of concrete material. The definition of the test is shown in Figure 8. More details of this particular test can be found in [8].

 Figure 8: Shear test in notched concrete specimen

The material properties for the DEM analysis are ${\textstyle E=35.5}$ GPa, ${\textstyle \nu =0,20}$, ${\textstyle \mu _{1}=0.1}$ and ${\textstyle \sigma _{t}^{f}=4.5}$ MPa. The analysis was carried out using 170k spherical particles. Figure 9 shows the load vertical displacement curve obtained with the DEM. Good agreement of the maximum load compared to the experimental value of 82,3 kN is obtained. Figure 10a show the multifracture pattern on the cylindrical sample at failure. The experimental results are displayed in Figure 10b.

 Figure 9: Shear test in notched concrete specimen. Load-displacement curve obtained with the DEM. Experimental failure load = 82,3 kN
 (a) (b) Figure 10: Shear test in concrete specimen. (a) DEM results. (b) Experimental results

The enhanced local DEM constitutive model can be used in conjunction with any constitutive law in solid mechanics for predicting the linear and non linear behavior of a solid. This opens the door for predicting with the DEM the linear and non linear response of solids and structures of any material (including metallic materias) [3], which is unusual for standard DEM models.

## 3. Interaction of discrete particles and solids modelled with the FEM

The interaction of discrete particles and solids can be studied by coupling the potential of the DEM and FEM approaches. Isolated particles can be modeled with the DEM, while solids are better modeled using the FEM. Indeed, complex objects can also be modeled using a collection of DEM particles, which allows one to use the standard frictional contact algorithms between particles and rigid/deformable objects developed for the DEM. Clearly, for rigid objects only the DEM particles discretizing the boundary of the object need to be accounted for.

The author's group has developed an innovative algorithms for modeling contact situations between discrete particles and solids modeled with the DEM [28]. The Double Hierarchy Method (termed ${\textstyle H^{2}}$) is a simple contact algorithm specially designed to resolve efficiently the intersection of spheres with triangles and planar quadrilaterals but it can also work well with any other higher order planar convex polyhedra. A two layer the hierarchy is applied upgrading the classical the hierarchy method presented by Horner et al. [12], namely hierarchy on type of contact followed by hierarchy on distance. The first hierarchy classifies the type of contact (facet, edge or vertex) for every contacting neighbour in a hierarchical way, while the distance-based hierarchy determines which of the contacts found are valid or relevant and which ones have to be removed.

The ${\textstyle H^{2}}$ algorithm has been developed taking into account its implementation in a parallel computing environment. This is particularly important for industrial problems involving a large number of particles interacting with a fine FEM mesh.

Summarizing, the ${\textstyle H^{2}}$ contact search satisfies the following requirements:

• Includes poly-disperse elements for both the FEM and the DEM.
• Allows different FE geometries and primitives (triangle, quadrilateral, polygon).
• Ensures contact continuity in non-smooth regions (edges and vertices).
• Resolve multiple contacts and contact with different entities simultaneously.
• Low memory storage.
• Simple, fast and accurate need.
• Fully parallelizable.

A simple particle-structure interaction example is presented next in order to assess the DEM-FEM coupling procedure. The example consists on a spherical particle colliding a simply supported beam (Figure 11). Two different cases are reproduced. The reference solution to this problem, taken from linear modal dynamics was proposed by Timoshenko [30] and is reviewed in [17].

The two examples are reproduced with the same DEM and FEM parameters. In the first one the particle radius is ${\textstyle 0.01\,m}$ and the length of the beam is ${\textstyle 15.35\,m}$, while in the second one the particle radius is ${\textstyle 0.02\,m}$ and the beam length is ${\textstyle 30.70\,m}$. The material properties and the simulation parameters are summarized in Table 3. The first case produces a single impact while the second yields three particle/beam impacts. The FEM meshes used are ${\textstyle 60\times 4\times 3}$ 8-nodded hexahedral elements respectively for the beam length, height and depth, respectively in the first example and ${\textstyle 120\times 4\times 3}$ hexahedra in the second example.

 Figure 11: Simply supported beam hit vertically at its centre by a sphere. (a) Front view. (b) Side view
 Material properties DEM Analysis parameters Sphere radius (${\textstyle m}$) ${\displaystyle 0.01/0.02}$ Density (${\textstyle kg/m^{3}}$) ${\displaystyle 7960}$ Young's modulus (${\textstyle GPa}$) ${\displaystyle 215.82}$ Initial velocity of sphere (${\textstyle m/s}$) ${\displaystyle \left[0.0,-0.01,0.0\right]}$ Poisson's ratio ${\displaystyle 0.289}$ Gravity (${\textstyle m/s^{2}}$) ${\displaystyle \left[0.0,0.0,0.0\right]}$ Friction parameter 0.0 Neighbour search freq. 50

The results shown in Figure 12 are quite satisfactory and the ${\textstyle H^{2}}$ model reproduces well the contact forces. Once the contact ends, the beam oscillates in a combination of different excited modes. The largest frequency mode, which can be easily identified in the figures, corresponds to the natural frequency of the beam and it is perfectly matched. The higher vibration modes however, are not correctly captured by the linear hexahedral elements, as they are not the best suited elements to simulate flexural modes. Consequently, there is a deviation on the second and third contact events in the second example (Figure 12b).

More details of this example and the ${\textstyle H^{2}}$ procedure can be found in [28,29].

 (a) Beam 1 (b) Beam 2 Figure 12: Lateral impact of a sphere on a simply supported beam. (a) Analytical solution versus DEM-FEM numerical solution for beam 1. (b) Analytical solution versus DEM-FEM numerical solution for the beam 2

### 3.1 A FEM-DEM procedure for multifracture analysis of solids

The DEM is a flexible method to simulate granular and non-continuum media, in particular the propagation of initial cracks. On the other hand, these contact properties are defined at the micro scale, while the material properties usually refer to experimental results in the macro scale. The step between both scales is not easy and requires a calibration task. The FEM otherwise is based in a continuum formulation involving the macro properties of the material. The FEM allows one to establish failure criteria compatible with the equilibrium equations in continuum mechanics, which makes it consistent and easy to apply for different materials.

The distance between DEM and FEM approaches is wide. Extensive research has been carried out in last years to combine FEM and DEM procedures, taking profit the advantages of both numerical methods. Combination of the FEM with the standard DEM using circular and spherical particles are reported in [13,20,22,27]. A combined finite-discrete element method based on the splitting of the finite elements into discrete elements of poligonal shape is presented in [10,11,18,19,20,23]. Zárate and Oñate [32,35] have recently presented a coupled FEM-DEM formulation for the numerical simulation of cracks starting from a finite element discretization of the domain.

The FEM-DEM formulation presented in [32,35] discretizes the continuum using linear 3-noded triangles (in 2D) and 4-noded tetrahedra (in 3D) whose nodes define the position of a (virtual) discrete element. These discrete elements are introduced in the simulation process when cracks appear. The normal contact forces between discrete elements are calculated integrating the stiffness matrix of the linear triangle along its sides that connect the discrete particles as shown in Figure 13 [32]. The mechanical problem in the crack-free region is solved using the standard FEM and an appropriate damage model. In the examples shown in this chapter damage onset and evolution of damage is governed by a Mohr-Coulomb failure criteria.

 Figure 13: Equivalence between stiffness matrix (FEM) and cohesive link (DEM)

Onset of a crack at the center of an element side depends on the damage level at that point. The stresses over the edge are computed as the mean of the stresses in the elements sharing that side.

Once the damage limit is reached, a stiffness loss is induced in the triangle. The stiffness loss is associated to the area determined by the centroid of the triangle and the damaged side as shown in Figure 14.

 Figure 14: Equivalence between stiffness matrix (FEM) and cohesive link (DEM) with a damaged edge

The stiffness matrix of a damaged element is recalculated at every time step as follows

 ${\displaystyle {K}^{(e)}=\left[1-{\frac {d_{i}+d_{j}}{2}}\right]{K}_{0}^{(e)}}$
(26)

where ${\textstyle {K}_{0}}$ is the initial stiffness matrix of the undamaged element and ${\textstyle d_{i}}$ and ${\textstyle d_{j}}$ are to the two maximum values of the damage parameters for the three element sides (Figure 15).

 Figure 15: Three-noded triangle with two sides damaged

When a cohesive bond is removed the side nodes of the element are disconnected and two discrete particles are introduced at the same nodal positions. Their radii and masses are defined as the maximum ones to guarantee contact without overlapping other discrete elements in order to avoid spurious contact forces [14].

Once the discrete elements are created their interaction is governed according to contact and friction laws, as in the general DEM formulation described in a previous section.

A relevant point in the FEM-DEM approach described above is its computational cost. Most of the cost in a DEM simulation is due to the contact searching algorithms. In the FEM-DEM technique presented the number of discrete elements is in general much lower than the number of nodes because the fractured area is typically smaller than the whole calculation domain. Hence, the computational time consumed by the contact searching algorithms is much lower than in a standard DEM solution.

### 3.2 Examples of application of the FEM-DEM procedure

#### Four-point bending beam

The 2D version of the FEM-DEM technique is applied to the study of the failure of a double notch concrete beam analyzed under plane stress conditions. The beam is supported at two points and deforms in a bending mode by imposing displacement at the two points depicted in Figure 16 where the beam dimensions are also shown.

 Figure 16: Double notched concrete beam. Dimensions and boundary conditions

Figure 17 shows the crack path obtained with the 2D FEM-DEM approach for the three meshes analysed which coincide with the numerical results of Cervera et al. [4]. The mix-mode fracture is clearly seen. Figure 18 shows the plots of the vertical reaction at a support version the imposed displacement at any of the two points depicted in Figure 16. The graphs are in good agreement with the results reported in [4].

 Figure 17: Double notched concrete beam. Displacement contours and crack path at the two notches regions using three different meshes of 3-noded triangles. (a) Coarse mesh (2202 triangles). (b) Intermediate mesh (3480 triangles). c) Fine mesh (11206 triangles). Discrete elements generated at the cracks
 ] Figure 18: Double notched concrete beam. Relationship between the force and the imposed displacement at any of the two points depicted in Figure 5. 3D FEM-DEM results are compared with those given in [4]

#### Brazilian tensile strength (BTS) test

We have applied the 3D FEM-DEM procedure to the simulation of a BTS test on a cylindrical concrete sample of diameter ${\textstyle D=0.2\,m}$ and ${\textstyle 0.1\,m}$ thickness (${\textstyle t}$). The tensile strength value is computed by [1]:

 ${\displaystyle f_{t}={\frac {2P}{\pi tD}}}$
(27)

were ${\textstyle P}$ is the applied load.

The material properties are ${\textstyle E_{o}=21}$ GPa, ${\textstyle \nu =0.2}$, ${\textstyle \gamma =7.8\times 10^{3}}$ N/m${\textstyle ^{3}}$, ${\textstyle f_{t}=10}$ KPa and ${\textstyle G_{f}=1\times 10^{-3}}$ J/m${\textstyle ^{2}}$. Using Eq.(27) this corresponds to a failure load of ${\textstyle P=314.16}$ N.

Three finite element meshes were used for the analysis with ${\textstyle 9338}$, ${\textstyle 31455}$ and ${\textstyle 61623}$ 4-noded linear tetrahedra, respectively. The crack patterns obtained for each mesh are depicted in Figure 19. The numerical results for the load-displacement curve are presented in Figure 20. The numerical values obtained for the tensile strength were (coarse to fine mesh) ${\textstyle 10693}$ Pa, ${\textstyle 10351}$ Pa and 10 235 Pa which yielded a range of ${\textstyle 6\%}$ to ${\textstyle 2\%}$ error versus the expected value of ${\textstyle f_{t}=10}$ kPa.

 Figure 19: 3D FEM-DEM analysis of BTS test on a concrete specimen. Damage zone and discrete elements generated. (a) Coarse mesh. (b) intermediate mesh. (c) Fine mesh
 Figure 20: 3D FEM-DEM analysis of BTS test on a concrete specimen. Force-displacement relationship for the three meshes used

#### Fracture of shale rock under a pulse load

The FEM-DEM procedure has been applied to the study of the fracture of a rock mass under a pulse load [9]. This is a usual procedure in the so-called fracking technique used in the oil and gas industry.

Figure 21 shows the geometry of the domain analyzed and the loads acting at the boundary. These loads are computed in terms of the depth of the rock mass analyzed. The evolution of the pulse load acting at central hole is shown in Figure 21. Figure 22 depicts the finite element mesh of 3-noded triangles used for the analysis. The fracture pattern in the rock obtained with the FEM-DEM technique for a depth of 500 ft are shown in Figure 23. The length of the vertical crack obtained is 36 ft which compares well with the length of 40 ft using the DEM [9] and also with an alternative FEM formulation [25].

 (a) (b) Figure 21: Fracture of shale rock. (a) Analysis domain and applied loads. (b) Pulse pressure function
 Figure 22: Shale rock domain under pulse load. Mesh of 3-noded triangles for FEM-DEM anaysis
 ] Figure 23: Crack simulation with FEM-DEM model. Depth 500 ft. FEM results in box from [25]

#### Multifracture of a tunnel front induced by a blast load

This example shows the capability of the FEM-DEM approach for simulating the evolution of multiple cracks in a tunnel front induced by a blast load.

Figure 24 shows the geometry of the front of the Bekkelaget tunnel in Norway, including the distribution of blast holes and the mesh of 38000 3-noded triangles discretizing the tunnel front. Details of the material properties, the blasting sequence and the computational features of this problem can be found in [34].

Figure 25 shows the evolution of cracks at the front induced by a particular blasting sequence. The results demonstrate the usefulness of the FEM-DEM technique for simulating this complex multifracturing problem.

 Figure 24: Distribution of blast holes at the front of the Bekkelaget tunnel (Norway) and finite element method for FEM-DEM simulation of the cracking pattern
 Figure 25: Evolution of cracking at the front of the Bekkelaget tunnel induced by a blasting sequence. FEM-DEM results

#### Fracture pattern in a granite rock specimen under pulse load accounting for the gas pressure

Figure 26 shows the fracture pattern in a cylindrical specimen of granite rock under a pulse load acting at the central hole. The effect of the gas filling the cracks has been taken into account by coupling the FEM-DEM procedure described earlier with a compressible flow FEM solver using an embedded solution technique. The coupling strategy solves the equations for the compressible gas flow in the finite element mesh that fills the spaces created by the cracks. Figure 26 shows a snapshot of the pressure field in the gas domain between the cracks at a certain instant. More information of this coupled solution can be found in [33].

 (a) (b) Figure 26: Fracture pattern in a cylindrical specimen of granite rock under an internal pulse load. FEM-DEM solution accounting for the effect of the gas filling the crackings. (a) Cracking pattern. (b) Pressure field in the gas domain within the cracks [33]

## Concluding remarks

This chapter has shown the possibility of the DEM for linear and non linear analysis of cohesive materials and structures, as well as the advantages of coupling the FEM and DEM techniques for studying the interaction of particles with structures and the prediction of complex multifracture situations in solids.

## Acknowledgements

This research was partially funded by the ICEBREAKER project of the European Research Council. Support for this work was also provided from the Office for Naval Research Global (ONRG) of the US Navy through the NICE-SHIP project. We also acknowledge the financial support of the CERCA programme of the Generalitat de Catalunya.

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Published on 01/01/2018

DOI: /10.1007/978-3-319-60885-3_15

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