Stability investigation of the Generalised-α time integration method for dynamic coupled consolidation analysis

Abstract In this paper, the stability of the Generalised-α time integration method (the CH method) for a fully coupled solid-pore fluid formulation is analytically investigated for the first time and the corresponding theoretical stability conditions are proposed based on a rigorous mathematical derivation process. The proposed stability conditions simplify to the existing ones of the CH method for the one-phase formulation when the solid–fluid coupling is ignored. Furthermore, by degrading the CH method to the Newmark method, the stability conditions are in agreement with the ones proposed in previous stability investigations on coupled formulation for the Newmark method. The analytically derived stability conditions are validated with finite element (FE) analyses considering a range of loading conditions and for various soil permeability values, showing that the numerical results are in agreement with the theoretical investigation. Then, the stability characteristics of the CH method are explored beyond the limits of the theoretical investigation, assuming elasto-plastic soil behaviour which is prescribed with a bounding surface plasticity constitutive model. Since the CH method is a generalisation of a number of other time integration methods, the derived stability conditions are relevant for most of the commonly utilised time integration methods for the two-phase coupled formulation.

[1]  J. C. Small,et al.  An investigation of the stability of numerical solutions of Biot's equations of consolidation , 1975 .

[2]  Achilleas G. Papadimitriou,et al.  Plasticity model for sand under small and large cyclic strains: a multiaxial formulation , 2002 .

[3]  A. Hurwitz Ueber die Bedingungen, unter welchen eine Gleichung nur Wurzeln mit negativen reellen Theilen besitzt , 1895 .

[4]  Lidija Zdravković,et al.  An assessment of time integration schemes for dynamic geotechnical problems , 2008 .

[5]  A. Chan A unified finite element solution to static and dynamic problems of geomechanics , 1988 .

[6]  D. Taborda Development of constitutive models for application in soil dynamics , 2011 .

[7]  Majidreza Nazem,et al.  Arbitrary Lagrangian–Eulerian method for dynamic analysis of geotechnical problems , 2009 .

[8]  W. L. Wood Practical Time-Stepping Schemes , 1990 .

[9]  Lidija Zdravković,et al.  Computational study on the modification of a bounding surface plasticity model for sands , 2014 .

[10]  H. Saunders,et al.  Finite element procedures in engineering analysis , 1982 .

[11]  Xikui Li,et al.  An iterative stabilized fractional step algorithm for finite element analysis in saturated soil dynamics , 2003 .

[12]  Nathan M. Newmark,et al.  A Method of Computation for Structural Dynamics , 1959 .

[13]  D. Potts,et al.  The Generalised-α Algorithm for Dynamic Coupled Consolidation Problems in Geotechnical Engineering , 2008 .

[14]  Lidija Zdravković,et al.  Seismic response and interaction of complex soil retaining systems , 2012 .

[15]  Majidreza Nazem,et al.  Large deformation dynamic analysis of saturated porous media with applications to penetration problems , 2014 .

[16]  Lidija Zdravković,et al.  Finite Element Analysis in Geotechnical Engineering: Theory , 1999 .

[17]  Thomas J. R. Hughes,et al.  Improved numerical dissipation for time integration algorithms in structural dynamics , 1977 .

[18]  T. Hughes,et al.  Collocation, dissipation and [overshoot] for time integration schemes in structural dynamics , 1978 .

[19]  O. C. Zienkiewicz,et al.  An alpha modification of Newmark's method , 1980 .

[20]  Jintai Chung,et al.  A Time Integration Algorithm for Structural Dynamics With Improved Numerical Dissipation: The Generalized-α Method , 1993 .

[21]  E. J. Routh A Treatise on the Stability of a Given State of Motion: Particularly Steady Motion , 2010 .