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Introduction to Discrete Element Modeling (DEM) simulation
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Debanga Nandan Mondal
Process and systems technology Laboratory, Åbo Akademi University, Biskopsgatan 8, FI-20500 Åbo, Finland
There are two kind of modeling approaches….Continuum
Constitutive Laws Substance is continuous &
fills the space it occupies Behavior of individual
particles is ignored constitutive equations are
solved numerically (e.g.Finite Element Method).
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Discrete Model each single particle Bulk = assembly of particles Individual particle ‐ particle
interaction investigating phenomena
occurring at the length scaleof particle diameter
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Continuum Discrete
Modeling of flows
Eulerian models –Reference frame outside
the motion of the constituents
–The fluid/particles are treated as continuum
–Bulk properties are required
–Boundary conditions are difficult to formulate
–Need to solve Navierstokes equation
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Lagrangian models –Reference frame moves along
with the constituent –The fluid/particles are
treated individually –Properties of individual
particles are needed –Boundary conditions are
relatively easier –Need to solve Newton’s
second law
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Eulerian models Lagrangian models
Modeling of flows
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Fluids
Granular particles
Single phase
Multi phase
fluid - fluid
fluid - particles
eulerian
lagrangian
Eulerian -eulerian
lagrangian -lagrangian
granular and fluid
granular
eulerian -eulerian
eulerian
lagrangian
eulerian -lagrangian
CFD
SPH, MPX
CFD
SPH, MPX
CFD-DEM
CFD-KT
KT, plasticity
DEM, MC
History
• 1956 : Alder and Wainwright: Theory of Discrete Element Model was
introduced : for Molecular dynamics
• 1970 : Cundall and Strack: The principles of discrete element
method : distinct element method
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Main principles of DEM
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1. Contact detection algorithms
2. Suitable contact models2.1. Accelerations2.2. Velocities2.3. Positions
Application of DEM Each particle in a system is tracked. Direct particle‐particle contact. Other contact forces can be implemented. Newton’s second law is solved
F=𝑚∙a Example of forces
–Contact forces –Gravitational force –Electrostatic or Magnetic force –Fluid drag force
The effect of the forces are integrated over time
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Main DEM parameters
Particle properties• Diameter• Density• Young’s modulus• Shear Modulus
Contact Properties• Coefficient of static friction• Coefficient of rolling friction
External Parameters• Gravity• Other forces (attraction & repulsion)
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Åbo Akademi University | Domkyrkotorget 3 | 20500 Åbo 11
Accelerations Velocities Positions Newton’s Laws
Contacts Forces Contact Mechanics
Discrete simulation approaches
Hard-sphere Interaction forces :
impulsiveMomentum exchange:
only particle collisions
18.10.2019Åbo Akademi University | Domkyrkotorget 3 | 20500 Åbo 12
Soft-sphereParticles are rigidSmall overlaps:
deformation duringcontact
Soft-sphere method is the mostcommonand accurate approach. It isused in most DEM packages, includingEDEM
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v1 v2
overlap
V1’ V2’
The soft‐sphere approach allows for small overlaps which are used to calculate magnitudes of the forces acting on particles.
Each particle within a granular flow has 6 degrees of freedom : Rotational and Translational motion
Newton’s second law is used to calculate the translational and rotational accelerations
Those are are then numerically integrated over a time step to update particle velocities and positions.
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Particle Motion Calculations
Particle Motion CalculationsRotation
I ω 𝑀
𝐼 : moment of inertia𝜔 : angular velocity𝑀 : resultant contact torque acting on the particle𝑡 : time
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mg
v
Fnc
Fc
M
ω
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Particle Motion Calculations
mg
v
Fnc
Fc
M
ω
Translation m 𝐹 𝐹 𝐹
v : translational velocity of the particlem : mass of the particle𝐹 : resultant gravitational force acting on the particle 𝐹 and 𝐹 : resultant contact and noncontact forces between the particle and surrounding particles or walls
Contact detection
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For spherical particles, a contact is detected if the distance between two spheres is less than summation of their radii
Computationally expensive
Borrowed from EDEM tutorial
Contact force models
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Borrowed from EDEM tutorial
There are few contact force models
The contact models are based on theories of contact mechanics and are mostly developed for spherical contacts.
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Spring dashpot contact model.
Cattaneo (1938) and Mindlin(1949) added tangential forces for slip conditions
Contact force models
Bubbling fluidized bed
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Fluent Discrete Phase Model with…
DEM collisions enabled
Macroscopic particle model
Particles are treated in a Lagrangian frame of reference.
Each particle is assumed to span several computational cells.
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Macroscopic particle model
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Fluid cells touched by particle and patching of particlevelocity
Borrowed from Macroscopic Particle ModelTracking Big Particles in CFD, Madhusuden Agrawal
Gas flow through coke bed
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CFD – DEM coupled
To study particle behavior in fluid phase.
Solid and fluid motions are solved through Newton’s equation of motion for discrete particles
Navier‐Stokes equation for continuum particles
Different drag models are applicable for particle‐fluid interaction
Coke bed descend: Different diameters
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How to simulate?
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Set: Particle properties
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Macroscopic Particle Model: ANSYS
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EDEM
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Particle dimension
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Build geometry
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Coke‐pellet descend
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Conclusions
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Discrete element modeling is becoming very powerful tools.
Computational limitations are disappearing everyday.
Parallel processing are making DEM calculations faster: by handling different particle motions at different processors.
Large particles are being simulated in CFD‐DEM coupled solvers.
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Heat transfer through particle bed can be calculated.
Forces acting on the containers and equipment can be calculated.
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References
Check any material about EDEM
Search google.
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