Bonding V2 Model

The Bonding V2 contact model is used to bond particles with a finite-sized 'glue' bond.

This bond can resist tangential and normal movement up to a maximum normal and tangential shear stress, at which point the bond breaks. Thereafter the particles interact as hard spheres. This model is based on the works of Potyondy and Cundall 2004. This model is particularly useful in modeling concrete and rock structures.


Bonds are created based on two methods - ‘current time’ or ‘fixed’. Once you have selected the Bonding V2 model, these options are displayed in the Factory creating the Bulk Material or Meta-Particles.
  • Current time allows the dynamic creation of bonded materials.
  • Fixed time allows the creation of bonded material at one user-defined point in time.

If the Bulk Material Active Bonds are defined and the Particles that comprise the Bulk Material are in contact at the bond creation time, the bonds are formed according the bond parameters. This occurs once per simulation for each particle pair. Once the bond time has passed, no new bonds will be formed.

You can also use a custom API factory to create material and use the Bonding V2 model. The API factory can be set to assign a Custom Property with the name CREATIONTIME = "Bond Creation Time”. The factory must then assign a value to the custom property equal to the current simulation time. EDEM will then create bonds between particles if the particles are in contact and both particles have a Custom Property CREATIONTIME value equal to the current simulation time. The custom property must be defined with 1 element and unit of eTime.

After bonding, the forces (Fn,t)/torques (Tn,t) on the particle are set to zero and are adjusted incrementally every Time Step as follows:

δ F n = − υ n S n A δ t MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiTdqMaam OramaaBaaaleaacaWGUbaabeaakiabg2da9iabgkHiTiabew8a1naa BaaaleaacaWGUbaabeaakiaadofadaWgaaWcbaGaamOBaaqabaGcca WGbbGaeqiTdqMaamiDaaaa@43D6@
δ F t = − υ t S t A δ t MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiTdqMaam OramaaBaaaleaacaWG0baabeaakiabg2da9iabgkHiTiabew8a1naa BaaaleaacaWG0baabeaakiaadofadaWgaaWcbaGaamiDaaqabaGcca WGbbGaeqiTdqMaamiDaaaa@43E8@
δ M n = − ω n S t J δ t MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiTdqMaam ytamaaBaaaleaacaWGUbaabeaakiabg2da9iabgkHiTiabeM8a3naa BaaaleaacaWGUbaabeaakiaadofadaWgaaWcbaGaamiDaaqabaGcca WGkbGaeqiTdqMaamiDaaaa@43F2@
δ M t = − ω t S n J 2 δ t MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiTdqMaam ytamaaBaaaleaacaWG0baabeaakiabg2da9iabgkHiTiabeM8a3naa BaaaleaacaWG0baabeaakiaadofadaWgaaWcbaGaamOBaaqabaGcda WcaaqaaiaadQeaaeaacaaIYaaaaiabes7aKjaadshaaaa@44C4@

Where

A = π R B 2 MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqaiabg2 da9iabec8aWjaadkfadaWgaaWcbaGaamOqaaqabaGcdaahaaWcbeqa aiaaikdaaaaaaa@3C3B@
J = 1 2 π R B 4 MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOsaiabg2 da9maalaaabaGaaGymaaqaaiaaikdaaaGaeqiWdaNaamOuamaaBaaa leaacaWGcbaabeaakmaaCaaaleqabaGaaGinaaaaaaa@3DCD@

RB is the radius of the glue. This value is set as the radius of the smallest particle out of a contact pair multiplied by the Bonded Disk Scale value that you have set.

Sn,t are the normal and shear stiffness respectively. If the Normal or Tangential Range value is set to 0 N/m3 then the stiffness value is assigned based on the bond configuration value. Otherwise the bond is assigned a value randomly distributed between the Stiffness value + or – the range value. This provides a linear distribution of bond stiffness values for a given material.

δt is the Time Step. vn,t are the normal and tangential velocities of the particles and ωn,t the normal and tangential angular velocities.

The bond is broken when the normal and tangential shear stresses exceed a predefined value.

σ max < − F n A + 2 M t J R B MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaS baaSqaaiGac2gacaGGHbGaaiiEaaqabaGccqGH8aapdaWcaaqaaiab gkHiTiaadAeadaWgaaWcbaGaamOBaaqabaaakeaacaWGbbaaaiabgU caRmaalaaabaGaaGOmaiaad2eadaWgaaWcbaGaamiDaaqabaaakeaa caWGkbaaaiaadkfadaWgaaWcbaGaamOqaaqabaaaaa@45C5@
τ max < − F t A + M n J R B MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiXdq3aaS baaSqaaiGac2gacaGGHbGaaiiEaaqabaGccqGH8aapdaWcaaqaaiab gkHiTiaadAeadaWgaaWcbaGaamiDaaqabaaakeaacaWGbbaaaiabgU caRmaalaaabaGaamytamaaBaaaleaacaWGUbaabeaaaOqaaiaadQea aaGaamOuamaaBaaaleaacaWGcbaabeaaaaa@450B@

These bond forces/torques are in addition to the Base Contact Model. Since the bonds involved in this model can act when the particles are no longer physically in contact, the contact radius must be set to higher than the actual radius of the spheres. This model may only be used between particles.

Select an active bond and then specify the Bond Formation method and the following parameters:

Interaction Configurable Parameters
Particle to Particle Normal Stiffness per unit area

Indicates the tensile/compressive stiffness along the bond’s principal axis.

Normal Range

Indicates the applied Normal Stiffness per unit area value assigned to the bond pair is a value randomly distributed between the Normal Stiffness value + or – the Normal range value.

Shear Stiffness per unit area

Indicates the Shear stiffness in the orthogonal plane to the bond’s principal axis.

Shear Range

Indicates the applied Shear Stiffness per unit area value assigned to the bond pair is a value randomly distributed between the Shear Stiffness value + or – the Shear range value.

Critical Normal Stress

Indicates the maximum normal stress the bond can withstand before it fails.

Critical Shear Stress

The maximum tangential stress the bond can withstand before it fails.

Bonded Disk Scale

The radius of the cylindrical bond between the particles will be equal to the smallest particle radius in a bond pair multiplied by the bonded disk scale value.

Torque Feedback
  • Enables the Bond Torque to be returned to the Particle.
  • Set the bond stress and stiffness values to represent the material that is been modeled. A high stiffness value will produce high bond forces and stresses. A lower than normal Time Step may be required to accurately capture these high forces.
  • When the Bond Formation Time is reached, all defined particles in contact will be bonded together. Before this time, particles interact based on the Hertz-Mindlin contact model.
  • A bond between two particles will cease to exist whenever one or both of the bonded particles leave the simulation domain. If periodic boundaries are applied when the particle leaves the domain, then the particle will exist on the opposite side of the domain; in this case the two particles will remain bonded across the periodic boundary.
  • When Torque Feedback is selected, the bonded structure has a greater resistance to bending when considering a bond between two spheres, for a bonded structure where rotation is limited this setting has less impact.