Impact of cylinder against a rigid wall: impactBar

Prepared by Philip Cardiff and Ivan Batistić


Tutorial Aims

  • Demonstrate how to perform a dynamic impact analysis with large deformations and large sliding contact.

Case Overview

In this case, which has been analysed by Cardiff et al. [1], a cylindrical copper bar impacts a rigid wall. The bar has an initial radius of \(r_0 = 3.2\) mm, an initial length of \(l_0 = 32.4\) mm, and an initial velocity of \(v_0 = 227\) m/s. A schematic of the problem geometry is shown in Figure 1. The problem is modelled as axisymmetric.

Geometry

Figure 1 - Problem geometry [1]

The mechanical properties are given in Table 1. Transient effects are included. A frictionless contact is considered between the rigid ground and the lower boundary of the cylinder. The model is solved in 1000 equally spaced time increments.

Table 1 - Mechanical properties

Parameter Symbol Value
Young's modulus \(E\) \(117\) GPa
Poisson's ratio \(\nu\) \(0.35\)
Initial yield stress \(\sigma_Y\) \(400\) MPa
Initial density $\rho$ $8930$ kg/m$^3$
Hardening modulus $\kappa$ $100$ MPa

Expected Results

The predicted deformed geometry is shown for four separate times in Figure 2. A comparison with the numerical results predicted by Aguirre et al. [2] is available in [1]. Table 2 compares the final end radius of the bar at \(80\) \(\mu\)s, for the finer mesh consisting of 5760 cells, with numerical results from other methodologies [2, 3]. Good agreement is found.

Geometry

Figure 2 - Predicted deformed geometry [1]

Table 2 - Predicted end radius at \(80\) \(\mu\)s.

Method Predicted radius (in mm)
[2] FE method - tetrahedra \(5.55\)
[2] FE method - hexahedra \(6.95\)
[2] FE method average nodal pressure \(6.99\)
[1] FV method \(6.98\)
solids4Foam $7.14$

Video 1 - Mesh deformation during impact, coloured by velocity

Running the Case

The tutorial case is located at solids4foam/tutorials/solids/elastoplasticity/impactBar. The case can be run using the included Allrun script, i.e. > ./Allrun.

The Allrun script first creates the blockMeshDict file from system/blockMeshDict.cylinder.m4 using the m4 scripting language. The blockMesh utility is then used to create the mesh. For foam-extend, the axis edges are manually removed using collapseEdges. The setFields utility initialises the old displacement and displacement-increment fields required by the time scheme at the beginning of the simulation. Finally, the case is run using the solids4Foam solver.


References

[1] P. Cardiff, Ž. Tuković, P. D. Jaeger, M. Clancy, and A. Ivanković, "A Lagrangian cell-centred finite volume method for metal forming simulation," International Journal for Numerical Methods in Engineering, vol. 109, no. 13, pp. 1777–1803, 2017.

[2] M. Aguirre, A. J. Gil, J. Bonet, and A. A. Carreño, "A vertex centred finite volume Jameson-Schmidt-Turkel (JST) algorithm for a mixed conservation formulation in solid dynamics," Journal of Computational Physics, vol. 259, pp. 672–699, 2014.

[3] J. Bonet and A. J. Burton, "A simple average nodal pressure tetrahedral element for incompressible and nearly incompressible dynamic explicit applications," Communications in Numerical Methods in Engineering, vol. 14, no. 5, pp. 437–449, 1998.