In the present paper one‐step implicit integration algorithms for the N‐body problem are developed. The time‐stepping schemes are based on a Petrov–Galerkin finite element method applied to the Hamiltonian formulation of the N‐body problem. The approach furnishes algorithmic energy conservation in a natural way. The proposed time finite element method facilitates a systematic implementation of a family of time‐stepping schemes. A particular algorithm is specified by the associated quadrature rule employed for the evaluation of time integrals. The influence of various standard as well as non‐standard quadrature formulas on algorithmic energy conservation and conservation of angular momentum is examined in detail for linear and quadratic time...
International audienceWe propose a new explicit pseudo-energy and momentum conserving scheme for the...
Most finite element packages use the Newmark algorithm for time integration of structural dynamics. ...
In the present paper two main research areas of computational mechanics, namely the finite element d...
In the present paper one‐step implicit integration algorithms for non‐linear elastodynamics are deve...
In the present paper a systematic development of higher order accurate time stepping schemes which e...
In this paper, we develop a finite element method for the temporal discretization of the equations o...
Abstract: This paper considers numerical methods in molecular dynamics. An overview of the...
Subcycling algorithms which employ multiple timesteps have been previously proposed for explicit dir...
The description of the symplectic multi-step algorithm for integration of the equations of motion wi...
The time-stepping finite-element method (FEM) has become a powerful tool in solving transient electr...
Recent developments have proved the advantage of combining both time implicit and time explicit inte...
In this note we suggest a new approach to ensure energy conservation in time-continuous finite eleme...
Abstract. The two-dimensional n-body problem of classical mechanics is a non-integrable Hamiltonian ...
Computational efficiency demands discretized, hierarchically organized and individually adaptive tim...
... serve stability. This article presents a new implicit time integrator, which is a particular app...
International audienceWe propose a new explicit pseudo-energy and momentum conserving scheme for the...
Most finite element packages use the Newmark algorithm for time integration of structural dynamics. ...
In the present paper two main research areas of computational mechanics, namely the finite element d...
In the present paper one‐step implicit integration algorithms for non‐linear elastodynamics are deve...
In the present paper a systematic development of higher order accurate time stepping schemes which e...
In this paper, we develop a finite element method for the temporal discretization of the equations o...
Abstract: This paper considers numerical methods in molecular dynamics. An overview of the...
Subcycling algorithms which employ multiple timesteps have been previously proposed for explicit dir...
The description of the symplectic multi-step algorithm for integration of the equations of motion wi...
The time-stepping finite-element method (FEM) has become a powerful tool in solving transient electr...
Recent developments have proved the advantage of combining both time implicit and time explicit inte...
In this note we suggest a new approach to ensure energy conservation in time-continuous finite eleme...
Abstract. The two-dimensional n-body problem of classical mechanics is a non-integrable Hamiltonian ...
Computational efficiency demands discretized, hierarchically organized and individually adaptive tim...
... serve stability. This article presents a new implicit time integrator, which is a particular app...
International audienceWe propose a new explicit pseudo-energy and momentum conserving scheme for the...
Most finite element packages use the Newmark algorithm for time integration of structural dynamics. ...
In the present paper two main research areas of computational mechanics, namely the finite element d...