Issue |
ESAIM: M2AN
Volume 59, Number 2, March-April 2025
|
|
---|---|---|
Page(s) | 729 - 748 | |
DOI | https://doi.org/10.1051/m2an/2025002 | |
Published online | 25 February 2025 |
Pseudo-energy-preserving explicit Runge–Kutta methods
1
Escuela de Ciencias Físicas y Matemáticas, Universidad de San Carlos de Guatemala, Guatemala City, Guatemala
2
Applied Mathematics and Computational Science, CEMSE Division, King Abdullah University of Science and Technology (KAUST), Thuwal 23955-6900, Kingdom of Saudi Arabia
3
Institute of Mathematics, Johannes Gutenberg University Mainz, Staudingerweg 9, 55130 Mainz, Germany
* Corresponding author: david.ketcheson@kaust.edu.sa
Received:
11
July
2024
Accepted:
12
January
2025
Using a recent characterization of energy-preserving B-series, we derive the explicit con- ditions on the coefficients of a Runge–Kutta method that ensure energy preservation (for Hamiltonian systems) up to a given order in the step size, which we refer to as the pseudo-energy-preserving (PEP) order. We study explicit Runge–Kutta methods with PEP order higher than their classical order. We provide examples of such methods up to PEP order six, and test them on Hamiltonian ODE and PDE systems. We find that these methods behave similarly to exactly energy-conservative methods over moderate time intervals and exhibit significantly smaller errors, relative to other Runge–Kutta methods of the same order, for moderately long-time simulations.
Mathematics Subject Classification: 65L06 / 65P10 / 37M15
Key words: Geometric integration / Hamiltonian systems / Runge–Kutta methods / energy preservation
© The authors. Published by EDP Sciences, SMAI 2025
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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