%0 Journal Article %1 lalegname2011wavecrack %A Lalegname, A. %A Sändig, A. %D 2011 %I Springer Netherlands %J International Journal of Fracture %K from:mhartmann ians imported vorlaeufig %N 2 %P 131--149 %R 10.1007/s10704-011-9650-6 %T Wave-crack interaction in finite elastic bodies %U http://dx.doi.org/10.1007/s10704-011-9650-6 %V 172 %X This paper continues studies in Lalegname et al. (Int J Fract 152:97--125, 2008 ) on crack propagation in a bounded linear elastic body under the influence of incident waves. In Lalegname et al. ( 2008 ) we have considered shear waves, whereas in this paper we discuss the influence of plane elastic waves to a running crack. Actually, the time dependent problem is formulated in a two-dimensional current cracked configuration by a system of linear elasto-dynamic equations. In order to describe the behaviour of the elastic fields near the straight crack tip, we transform these equations to a reference configuration and derive the dynamic stress singularities. Furthermore, we assume that an energy balance law is valid. Exploiting the knowledge on the singular behaviour of the crack fields, we derive from the energy balance law a dynamic energy release rate. Comparing this energy release rate with an experimentally given fracture toughness we get an ordinary differential equation for the crack tip motion. We present first numerical simulations for a Mode I crack propagation.

@article{lalegname2011wavecrack, abstract = {This paper continues studies in Lalegname et al. (Int J Fract 152:97--125, 2008 ) on crack propagation in a bounded linear elastic body under the influence of incident waves. In Lalegname et al. ( 2008 ) we have considered shear waves, whereas in this paper we discuss the influence of plane elastic waves to a running crack. Actually, the time dependent problem is formulated in a two-dimensional current cracked configuration by a system of linear elasto-dynamic equations. In order to describe the behaviour of the elastic fields near the straight crack tip, we transform these equations to a reference configuration and derive the dynamic stress singularities. Furthermore, we assume that an energy balance law is valid. Exploiting the knowledge on the singular behaviour of the crack fields, we derive from the energy balance law a dynamic energy release rate. Comparing this energy release rate with an experimentally given fracture toughness we get an ordinary differential equation for the crack tip motion. We present first numerical simulations for a Mode I crack propagation.}, added-at = {2018-07-20T10:55:00.000+0200}, affiliation = {Institute of Applied Analysis and Numerical Simulation, University of Stuttgart, Pfaffenwaldring 57, 70569 Stuttgart, Germany}, author = {Lalegname, A. and S{\"a}ndig, A.}, biburl = {https://puma.ub.uni-stuttgart.de/bibtex/27e3434e7e06a854b0b106cd2ec5f2238/mathematik}, doi = {10.1007/s10704-011-9650-6}, interhash = {605386b138c61d78fb45cc0b73405a20}, intrahash = {7e3434e7e06a854b0b106cd2ec5f2238}, issn = {0376-9429}, journal = {International Journal of Fracture}, keyword = {Chemie und Materialwissenschaften}, keywords = {from:mhartmann ians imported vorlaeufig}, note = {10.1007/s10704-011-9650-6}, number = 2, pages = {131--149}, publisher = {Springer Netherlands}, timestamp = {2019-12-18T14:37:55.000+0100}, title = {Wave-crack interaction in finite elastic bodies}, url = {http://dx.doi.org/10.1007/s10704-011-9650-6}, volume = 172, year = 2011 }