Abstract:In quasistatic solid mechanics the spatial as well as the temporal domain need to be discetized. For the spatial discretization usually elements with linear shape functions are used even though it has been shown that generally the p‐version of the finite elemente method yields more effective discretizations, see e.g. [1], [2]. For the temporal discretization diagonal‐implicit, see e.g. [4], and especially linear‐implicit Runge‐Kutta schemes, see e.g. [5], [6], have for smooth problems proven to be superior to … Show more
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