Inclusion of Non-Conservative Forces in Geometric Integrators with Application to Orbit–Attitude Coupling

2021 ◽  
pp. 1-14
Author(s):  
Dante A. Bolatti ◽  
Anton H. J. de Ruiter
2009 ◽  
Vol 20 (02) ◽  
pp. 313-322
Author(s):  
PILWON KIM

Numerical schemes that are implemented by interpolation of exact solutions to a differential equation naturally preserve geometric properties of the differential equation. The solution interpolation method can be used for development of a new class of geometric integrators, which generally show better performances than standard method both quantitatively and qualitatively. Several examples including a linear convection equation and a nonlinear heat equation are included.


1997 ◽  
Vol 133 (1) ◽  
pp. 160-172 ◽  
Author(s):  
Jason Frank ◽  
Weizhang Huang ◽  
Benedict Leimkuhler

Author(s):  
Dina Razafindralandy ◽  
Aziz Hamdouni ◽  
Marx Chhay

2021 ◽  
Vol 155 (12) ◽  
pp. 124104
Author(s):  
Seonghoon Choi ◽  
Jiří Vaníček

2021 ◽  
pp. 313-420
Author(s):  
Grigori N. Milstein ◽  
Michael V. Tretyakov

SIMULATION ◽  
2019 ◽  
Vol 95 (11) ◽  
pp. 1055-1067
Author(s):  
Guillaume Chauvon ◽  
Philippe Saucez ◽  
Alain Vande Wouwer

Geometric integrators allow preservation of specific geometric properties of the exact flow of differential equation systems, such as energy, phase-space volume, and time-reversal symmetry, and are particularly reliable for long-run integration. In this study, variable step size composition methods and Gauss methods are implemented in Matlab library integrators, and are tested with several representative problems, including the Kepler problem, the outer solar system and a conservative Lotka–Volterra system. Variable step size integrators often perform better than their fixed step size counterparts and the numerical results show excellent long time preservation of the Hamiltonian in these examples.


2013 ◽  
Vol 11 (01) ◽  
pp. 1450009 ◽  
Author(s):  
ASIF MUSHTAQ ◽  
ANNE KVÆRNØ ◽  
KÅRE OLAUSSEN

We discuss systematic extensions of the standard (Störmer–Verlet) method for integrating the differential equations of Hamiltonian mechanics. Our extensions preserve the symplectic geometry exactly, as well as all Nöether conservation laws caused by joint symmetries of the kinetic and potential energies (like angular momentum in rotation invariant systems). These extensions increase the accuracy of the integrator, which for the Störmer–Verlet method is of order τ2 for a timestep of length τ, to higher-orders in τ. The schemes presented have, in contrast to most previous proposals, all intermediate timesteps real and positive. The schemes increase the relative accuracy to order τN (for N = 4, 6 and 8) for a large class of Hamiltonian systems.


2009 ◽  
Author(s):  
Elena Celledoni ◽  
Robert I. McLachlan ◽  
Brynjulf Owren ◽  
G. R. W. Quispel ◽  
Theodore E. Simos ◽  
...  

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