Section 6: Material modelling in solid mechanics - GAMM 2012
Section 6: Material modelling in solid mechanics - GAMM 2012
Section 6: Material modelling in solid mechanics - GAMM 2012
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8 <strong>Section</strong> 6: <strong>Material</strong> <strong>modell<strong>in</strong>g</strong> <strong>in</strong> <strong>solid</strong> <strong>mechanics</strong><br />
First the macroscale constitutive model based on the cont<strong>in</strong>uum theory of dislocations [1,2]<br />
is discussed. The plastic deformation and crack growth dur<strong>in</strong>g ductile fracture mutually effect<br />
each other, where dislocations’ movement shape the crack growth, and the latter effects the<br />
dislocations density [3]. We discuss the numerical implementation of the proposed crystal viscoelastoplasticity<br />
model coupled with modern dislocation measures [1,2] and present an example<br />
where the mechanisms of crystal plasticity are l<strong>in</strong>ked to the ductile fracture. The results focus<br />
the effect of severe plastic deformation on dislocations evolution and crack growth behaviour,<br />
follow<strong>in</strong>g the approach of Cherepanov [3].<br />
[1] T. Hochra<strong>in</strong>er, M. Zaiser, P. Gumbsch, A three-dimensional cont<strong>in</strong>uum theory of dislocation<br />
systems: k<strong>in</strong>ematics and mean-field formulation, Philosophical Magaz<strong>in</strong>e, 87:8-9 (2007),<br />
1261-1282.<br />
[2] S. Sandfeld, T. Hochra<strong>in</strong>er, P. Gumbsch, M. Zaiser, Numerical implementation of a 3D<br />
cont<strong>in</strong>uum theory of dislocation: dynamics and application to micro-bend<strong>in</strong>g, Philosophical<br />
Magaz<strong>in</strong>e, 90:27-28 (2010), 3697-3728.<br />
[3] G.P. Cherepanov et al., Dislocation generation and crack growth under monotonic load<strong>in</strong>g,<br />
J. Appl. Phys., 78(10) (1995), 6249-6264.<br />
Multiscale <strong>modell<strong>in</strong>g</strong> and simulation of micro mach<strong>in</strong><strong>in</strong>g of titan<br />
Richard Lohkamp, Ralf Müller (TU Kaiserslautern)<br />
The topology of micro mach<strong>in</strong>ed surfaces depends strongly on the underly<strong>in</strong>g heterogeneous microstructure<br />
of the material. The crystal structure <strong>in</strong>fluences the deformation and separation<br />
characteristics. In the case of α-titanium the deformation is dictated by the hcp crystal structure<br />
with its specific slip systems. In the crystal plastic deformation it is essential to take self and latent<br />
harden<strong>in</strong>g <strong>in</strong>to account. Furthermore to capture the rate dependent behavior a visco-plastic<br />
evolution law is used. This sett<strong>in</strong>g serves as a framework for more complex constitutive laws, such<br />
as the one given <strong>in</strong> [1].<br />
As a first attempt to model the cutt<strong>in</strong>g process, the fracture mechanisms <strong>in</strong> a crystall<strong>in</strong>e αtitanium<br />
are analysed with<strong>in</strong> the concept of configurational forces. To this end the theory of<br />
configurational forces is presented for a standard dissipative medium and is specialized to the<br />
crystal plasticity sett<strong>in</strong>g. The numerical implementation of the material law and the configurational<br />
forces is done <strong>in</strong> a consistent way with<strong>in</strong> the f<strong>in</strong>ite element method. The application of<br />
configurational forces <strong>in</strong> the crystal plasticity sett<strong>in</strong>g is discussed and demonstrated by illustrative<br />
examples.<br />
S6.4: Polymers and Elastomers II Tue, 16:00–18:00<br />
Chair: Alexander Lion, Joachim Schmitt S1|01–A1<br />
How to approximate the <strong>in</strong>verse Langev<strong>in</strong> function?<br />
Mikhail Itskov, Roozbeh Dargazany, Karl Hörnes (RWTH Aachen)<br />
The <strong>in</strong>verse Langev<strong>in</strong> function directly results from the non-Gaussian theory of rubber elasticity<br />
as the cha<strong>in</strong> force and represents an <strong>in</strong>dispensable <strong>in</strong>gredient of full-network rubber elasticity models.<br />
However, the <strong>in</strong>verse Langev<strong>in</strong> function cannot be represented <strong>in</strong> a closed-form and requires<br />
an approximation as for example a Padé approximation. The Padé approximations can be given