PreprintCC BY 4.0arXiv
A structure-preserving implicit-explicit method for a hyperbolic approximation of fourth-order PDEs
Abstract
We introduce a novel structure-preserving numerical method for a first-order hyperbolic approximation system, which approximates the solutions of general fourth-order partial differential equations. By employing an implicit-explicit (IMEX) splitting between the stiff and non-stiff terms, we rigorously prove that the proposed scheme is energy-consistent and positivity-preserving under a CFL-type condition. Furthermore, we show that the method remains robustly stable in asymptotic regimes, with a time-step restriction that is entirely independent of the relaxation parameters. Finally, we present a series of numerical examples for thin film equations to validate the theoretical properties and efficacy of the scheme.
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BibTeX
@misc{barthwal2026structurepreserving,
title = {{A structure-preserving implicit-explicit method for a hyperbolic approximation of fourth-order PDEs}},
author = {Rahul Barthwal and Rahuldev Ghorai},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.05939},
eprint = {2609.05939},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.05939},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - A structure-preserving implicit-explicit method for a hyperbolic approximation of fourth-order PDEs
AU - Rahul Barthwal
AU - Rahuldev Ghorai
PY - 2026
DA - 2026/09/05
PB - arXiv
DO - 10.48550/arxiv.2609.05939
UR - https://arxiv.org/abs/2609.05939
AB - We introduce a novel structure-preserving numerical method for a first-order hyperbolic approximation system, which approximates the solutions of general fourth-order partial differential equations. By employing an implicit-explicit (IMEX) splitting between the stiff and non-stiff terms, we rigorously prove that the proposed scheme is energy-consistent and positivity-preserving under a CFL-type condition. Furthermore, we show that the method remains robustly stable in asymptotic regimes, with a time-step restriction that is entirely independent of the relaxation parameters. Finally, we present a series of numerical examples for thin film equations to validate the theoretical properties and efficacy of the scheme.
ER -