Quasi-Orthogonal Runge-Kutta Projection Methods
A wide range of physical phenomena exhibit auxiliary admissibility criteria, such as conservation of entropy or various energies, which arise implicitly under exact solution of their governing PDEs. However, standard temporal schemes, such as classical Runge-Kutta (RK) methods, do not enforce these...
Gespeichert in:
Hauptverfasser: | , |
---|---|
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | A wide range of physical phenomena exhibit auxiliary admissibility criteria,
such as conservation of entropy or various energies, which arise implicitly
under exact solution of their governing PDEs. However, standard temporal
schemes, such as classical Runge-Kutta (RK) methods, do not enforce these
constraints, leading to a loss of accuracy and stability. Projection is an
efficient way to address this shortcoming by correcting the RK solution at the
end of each time step. Here we introduce a novel projection method for explicit
RK schemes, called a \textit{quasi-orthogonal} projection method. This method
can be employed for systems containing a single (not necessarily convex)
invariant functional, for dissipative systems, and for the systems containing
multiple invariants. It works by projecting the orthogonal search direction(s)
into the solution space spanned by the RK stage derivatives. With this approach
linear invariants of the problem are preserved, the time step size remains
fixed, additional computational cost is minimal, and these optimal search
direction(s) preserve the order of accuracy of the base RK method. This
presents significant advantages over existing projection methods. Numerical
results demonstrate that these properties are observed in practice for a range
of applications. |
---|---|
DOI: | 10.48550/arxiv.2409.18328 |