Increasing the critical time step: micro-inertia, inertia penalties and mass scaling
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[1] J. Huetink,et al. Simulation of aluminium sheet forming at elevated temperatures , 2006 .
[2] A. Eringen. On differential equations of nonlocal elasticity and solutions of screw dislocation and surface waves , 1983 .
[3] J. Awrejcewicz,et al. Asymptotic approaches in mechanics: New parameters and procedures , 2003 .
[4] Antonio Rodríguez-Ferran,et al. Bipenalty method for time domain computational dynamics , 2010, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.
[5] H. Askes,et al. Element size and time step selection procedures for the numerical analysis of elasticity with higher-order inertia , 2008 .
[6] R. D. Mindlin. Micro-structure in linear elasticity , 1964 .
[7] Jacob Fish,et al. Non‐local dispersive model for wave propagation in heterogeneous media: one‐dimensional case , 2002 .
[8] Harm Askes,et al. The Representative Volume Size in Static and Dynamic Micro-Macro Transitions , 2005 .
[9] Julius Kaplunov,et al. On Timoshenko-Reissner type theories of plates and shells , 1993 .
[10] Mattias Unosson,et al. Selective mass scaling for explicit finite element analyses , 2005 .
[11] Eiji Nakamachi,et al. Dynamic‐explicit elastic plastic finite‐element simulation of hemispherical punch‐drawing of sheet metal , 1996 .
[12] Lars Olovsson,et al. Iterative solution technique in selective mass scaling , 2005 .
[13] M. B. Rubin,et al. Continuum model of dispersion caused by an inherent material characteristic length , 1995 .
[14] Jeong Kim,et al. A comparative study of implicit and explicit FEM for the wrinkling prediction in the hydroforming process , 2003 .
[15] B. H. Aubert,et al. A mass penalty technique to control the critical time increment in explicit dynamic finite element analyses , 1995 .
[16] Shaoqun Zeng,et al. The key technology and realization of virtual ring rolling , 2007 .
[17] A. Tyas,et al. Asymptotic equivalence of homogenisation procedures and fine-tuning of continuum theories , 2008 .
[18] J. Fish,et al. A Dispersive Model for Wave Propagation in Periodic Heterogeneous Media Based on Homogenization With Multiple Spatial and Temporal Scales , 2001 .
[19] C. Sun,et al. Modeling micro-inertia in heterogeneous materials under dynamic loading , 2002 .
[20] Graeme W Milton,et al. On modifications of Newton's second law and linear continuum elastodynamics , 2007, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.
[21] J. Awrejcewicz,et al. Continuous models for 2D discrete media valid for higher-frequency domain , 2008 .
[22] Petr Plechác,et al. Implicit Mass-matrix Penalization of Hamiltonian Dynamics with Application to Exact Sampling of Stiff Systems , 2009, Multiscale Model. Simul..
[23] Andrei V. Metrikine,et al. An isotropic dynamically consistent gradient elasticity model derived from a 2D lattice , 2006 .
[24] J. Awrejcewicz,et al. Continuous models for 1D discrete media valid for higher-frequency domain , 2005 .
[25] H. Askes,et al. Penalty methods for time domain computational dynamics based on positive and negative inertia , 2009 .
[26] Mattias Unosson,et al. Selective mass scaling for thin walled structures modeled with tri-linear solid elements , 2004 .
[27] J. Engelbrecht,et al. Waves in microstructured materials and dispersion , 2005 .
[28] H. Askes,et al. One-dimensional dynamically consistent gradient elasticity models derived from a discrete microstructure: Part 2: Static and dynamic response , 2002 .
[29] Andrei V. Metrikine,et al. One-dimensional dynamically consistent gradient elasticity models derived from a discrete microstructure: Part 1: Generic formulation , 2002 .
[30] Ted Belytschko,et al. On the dynamic effects of explicit FEM in sheet metal forming analysis , 1998 .
[31] E. Aifantis,et al. On the role of microstructure in the behavior of soils: Effects of higher order gradients and internal inertia , 1994 .