SphericalParticleCohesiveForce< dim, number, ObstacleType > Class Template Reference
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Developer Documentation
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#include <cohesive_forces.hpp>
Classes | |
| struct | CohesiveContactConfiguration |
Public Member Functions | |
| SphericalParticleCohesiveForce (const SphericalParticleCohesiveForceData< number > &cohesive_force_data) | |
| void | add_load_to_obstacles (ObstacleField< dim, number, ObstacleType > &obstacle_field) const |
Private Attributes | |
| SphericalParticleCohesiveForceData< number > | cohesive_force_data |
| Cohesive force data for the spherical particle cohesive force model. | |
Constructor & Destructor Documentation
◆ SphericalParticleCohesiveForce()
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explicit |
Constructor for the spherical particle cohesive force model.
- Parameters
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cohesive_force_data Cohesive force data defining the material and cohesive contact properties.
Member Function Documentation
◆ add_load_to_obstacles()
| void MeltPoolDG::SphericalParticleCohesiveForce< dim, number, ObstacleType >::add_load_to_obstacles | ( | ObstacleField< dim, number, ObstacleType > & | obstacle_field | ) | const |
Computes the total cohesive load acting on all particles in a given obstacle field. The formulation follows Meier et al. (DOI:10.1016/j.powtec.2018.11.072). The resulting forces are accumulated and directly applied to the particles contained in the obstacle field.
For the computation of the cohesive force between two particles, three interaction regimes are distinguished based on their surface-to-surface distance.
For particles in close contact, i.e., if the surface-to-surface distance is smaller than \(g_0\), a constant pull-off force based on the DMT model is applied:
\[ \boldsymbol{F}_{\mathrm{po}} = 4 \pi R_e \gamma \boldsymbol{N}, \]
where \(R_e\) is the effective radius, \(\gamma\) the surface energy, and \(\boldsymbol{N}\) the unit normal vector pointing from one particle to the other. The characteristic distance \(g_0\) is given by
\[ g_0 = \sqrt{\frac{A R_e}{6 \lVert \boldsymbol{F}_{\mathrm{po}} \rVert}}. \]
If the surface-to-surface distance is larger than \(g_0\) but smaller than the cut-off distance \(g^*\), the cohesive force is computed as
\[ \boldsymbol{F} = \frac{A R_e}{6 g_N^2} \boldsymbol{N}, \]
where \(A\) is the Hamaker constant and \(g_N\) the surface-to-surface distance. The cut-off distance is defined as
\[ g^* = \frac{g_0}{\sqrt{c_{\mathrm{FPO}}}}, \]
where \(c_{\mathrm{FPO}}\) denotes the relative cut-off decline of the van der Waals force.
For surface-to-surface distances larger than the cut-off distance \(g^*\), no cohesive forces are applied.
- Parameters
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obstacle_field Obstacle field containing the particles for which cohesive forces are computed. The resulting forces are added directly to the particles in this field.
Member Data Documentation
◆ cohesive_force_data
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private |
Cohesive force data for the spherical particle cohesive force model.
The documentation for this class was generated from the following files:
- include/meltpooldg/particles/cohesive_forces.hpp
- source/particles/cohesive_forces.cpp
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