Merge pull request #135 from KratosMultiphysics/mpm/change-application-name

[MPM] Change application name

Author: ncrescenzio

README.md

@@ -130,11 +130,11 @@ Unit tests should *not* be uploaded to this repository. Please put them in the `
 - [Small Box Lagrangian OW](swimming_dem_fluid_interaction/use_cases/PFEMFluid_Element/One_Way/Small_Box_Eulerian_OW/README.md)
 - [Small Box Lagrangian TW](swimming_dem_fluid_interaction/use_cases/PFEMFluid_Element/Two_Way/Small_Box_Eulerian_TW/README.md)
 
-## Particle Mechanics
+## MPM (Material Point Method)
 
 **Validation**
-- [Granular Flow 2D](particle_mechanics/validation/granular_flow_2D/README.md)
-- [Cylinder on inclined plane 2D](particle_mechanics/validation/cylinder_on_inclined_plane/README.md)
+- [Granular Flow 2D](mpm/validation/granular_flow_2D/README.md)
+- [Cylinder on inclined plane 2D](mpm/validation/cylinder_on_inclined_plane/README.md)
 
 ## PFEM2
 

particle_mechanics/README.md mpm/README.mdparticle_mechanics/README.md renamed to mpm/README.md

@@ -1,11 +1,11 @@
-# Particle Mechanics Examples
+# Material Point Method (MPM) Examples
 
-This folder contains examples related to the [Particle Mechanics Application](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/ParticleMechanicsApplication) implemented in Kratos-Multiphysics. 
+This folder contains examples related to the [MPM Application](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/MPMApplication) implemented in Kratos-Multiphysics.
 
 ## Instruction
-- Please follow the instruction to download and install the latest version of the application and the GiD interface, [here](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/ParticleMechanicsApplication). 
+- Please follow the instruction to download and install the latest version of the application and the GiD interface, [here](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/MPMApplication).
 - At the moment, we only support [GiD](https://www.gidhome.com/) for pre- and post-processing.
-- For unit testings of the currently available feature, please visit the [tests](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/ParticleMechanicsApplication/tests) folder in Particle Mechanics Application.
+- For unit testings of the currently available feature, please visit the [tests](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/MPMApplication/tests) folder in MPM Application.
 
 ## Examples
 

particle_mechanics/use_cases/README.md mpm/use_cases/README.mdparticle_mechanics/use_cases/README.md renamed to mpm/use_cases/README.md

@@ -1,20 +1,20 @@
 # Cylinder on inclined plane 2D - comparison between analytical and numerical solution with MPM
-**Author:** Philip Franz 
+**Author:** Philip Franz
 
-**Kratos version:** Development branch. **Expected 9.1** 
+**Kratos version:** Development branch. **Expected 9.1**
 
-**Source files:** [cylinder_on_inclined_plane_2D](https://github.com/KratosMultiphysics/Examples/tree/master/particle_mechanics/validation/cylinder_on_inclined_plane/source)
+**Source files:** [cylinder_on_inclined_plane_2D](https://github.com/KratosMultiphysics/Examples/tree/master/mpm/validation/cylinder_on_inclined_plane/source)
 
 
 
 ## Case Specification
 
-This is a 2D simulation of a cylinder on an inclined plane. A rotating as well as a frictionless sliding behaviour of the cylinder are regarded subsequently. The simulation is set up according to section 4.5.2 of (Iaconeta, 2019). 
+This is a 2D simulation of a cylinder on an inclined plane. A rotating as well as a frictionless sliding behaviour of the cylinder are regarded subsequently. The simulation is set up according to section 4.5.2 of (Iaconeta, 2019).
 Linear, unstructured, triangular elements with a size of 0.01m are used to initialize the MPs. Three MPs per cell are considered. For the backgroundmesh linear, unstructured, triangular elements with a size of 0.02m are used.
-However, in contrast to section 4.5.2 of (Iaconeta, 2019), the inclined plane is modelled by a line with unstructured elements with size 0.01m. On that line a non conforming Dirichlet boundary condition is imposed by using the penalty method based on (Chandra et al., 2021).  
+However, in contrast to section 4.5.2 of (Iaconeta, 2019), the inclined plane is modelled by a line with unstructured elements with size 0.01m. On that line a non conforming Dirichlet boundary condition is imposed by using the penalty method based on (Chandra et al., 2021).
 
 The following applications of Kratos are used:
-- [ParticleMechanicsApplication](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/ParticleMechanicsApplication)
+- [MPMApplication](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/MPMApplication)
 - [LinearSolversApplication](https://github.com/KratosMultiphysics/Kratos/tree/master/applications/LinearSolversApplication)
 
 The problem geometry as well as the boundary conditions are sketched below. The non conforming boundary condition is respresented by the copper coloured line.
@@ -28,7 +28,7 @@ A hyper elastic Neo Hookean Plane strain (2D) constitutive law with unit thickne
 * Young's modulus (_E_):  200 MPa
 * Poisson ratio (_ν_): 0.3
 
-The time step is 0.001 seconds; the total simulation time is 1.0 seconds. The angle (_α_) of the inclined plane is 60°. The penalty-factor is 1e13. 
+The time step is 0.001 seconds; the total simulation time is 1.0 seconds. The angle (_α_) of the inclined plane is 60°. The penalty-factor is 1e13.
 
 The contact between cylinder and inclined plane is modelled with the option "contact" (see line 53, file *ProjectParameters_contact.json*) in the first and with "slip" in the second case, based on (Chandra et al., 2021). Choosing "contact" leads to a rolling behaviour of the cylinder; "slip" to frictionless sliding.
 
@@ -51,7 +51,7 @@ The left image displays the rolling cylinder - modelled with option "contact". T
 
 
 
- 
+
 ## References
-- Iaconeta, I. (2019). *Discrete-continuum hybrid modelling of flowing and static regimes.* (Ph.D. thesis). Universitat politècnica de Catalunya - Barcelona tech 
-- Chandra, B., Singer, V., Teschemacher, T., Wüchner, R., Larese, A. (2021) *Nonconforming Dirichlet boundary conditions in implicit material point method by means of penalty augmentation*. Acta Geotech. 16, 2315–2335. https://doi.org/10.1007/s11440-020-01123-3 
+- Iaconeta, I. (2019). *Discrete-continuum hybrid modelling of flowing and static regimes.* (Ph.D. thesis). Universitat politècnica de Catalunya - Barcelona tech
+- Chandra, B., Singer, V., Teschemacher, T., Wüchner, R., Larese, A. (2021) *Nonconforming Dirichlet boundary conditions in implicit material point method by means of penalty augmentation*. Acta Geotech. 16, 2315–2335. https://doi.org/10.1007/s11440-020-01123-3

particle_mechanics/validation/README.md mpm/validation/README.mdparticle_mechanics/validation/README.md renamed to mpm/validation/README.md

@@ -0,0 +1,16 @@
+import KratosMultiphysics
+from KratosMultiphysics.MPMApplication.mpm_analysis import MPMAnalysis
+
+"""
+For user-scripting it is intended that a new class is derived
+from MPMAnalysis to do modifications
+"""
+
+if __name__ == "__main__":
+
+    with open("ProjectParameters_contact.json",'r') as parameter_file:
+        parameters = KratosMultiphysics.Parameters(parameter_file.read())
+
+    model = KratosMultiphysics.Model()
+    simulation = MPMAnalysis(model,parameters)
+    simulation.Run()