Low-storage implicit/explicit Runge–Kutta schemes for the simulation of stiff high-dimensional ODE systems
Implicit/explicit (IMEX) Runge–Kutta (RK) schemes are effective for time-marching ODE systems with both stiff and nonstiff terms on the RHS; such schemes implement an (often A-stable or better) implicit RK scheme for the stiff part of the ODE, which is often linear, and, simultaneously, a (more conv...
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Veröffentlicht in: | Journal of computational physics 2015-04, Vol.286, p.172-193 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Implicit/explicit (IMEX) Runge–Kutta (RK) schemes are effective for time-marching ODE systems with both stiff and nonstiff terms on the RHS; such schemes implement an (often A-stable or better) implicit RK scheme for the stiff part of the ODE, which is often linear, and, simultaneously, a (more convenient) explicit RK scheme for the nonstiff part of the ODE, which is often nonlinear. Low-storage RK schemes are especially effective for time-marching high-dimensional ODE discretizations of PDE systems on modern (cache-based) computational hardware, in which memory management is often the most significant computational bottleneck. In this paper, we develop and characterize eight new low-storage implicit/explicit RK schemes which have higher accuracy and better stability properties than the only low-storage implicit/explicit RK scheme available previously, the venerable second-order Crank–Nicolson/Runge–Kutta–Wray (CN/RKW3) algorithm that has dominated the DNS/LES literature for the last 25 years, while requiring similar storage (two, three, or four registers of length N) and comparable floating-point operations per timestep. |
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ISSN: | 0021-9991 1090-2716 |
DOI: | 10.1016/j.jcp.2015.01.031 |