Energy conservation uncertainly due to the use of an implicit time integration method clarified by a multiplexed TGV inviscid flow

This study attempts to elucidate the conservation errors induced by the implicit time integration method within a multiscale flow. Using the multiplexed Taylor analytical solution as the initial field, three distinct multiscale turbulence fields were formulated, each characterised by different waven...

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Published inJournal of physics. Conference series Vol. 2701; no. 1; pp. 12059 - 12064
Main Authors Chitose, Makoto, Suzuki, Hiroki, Kouchi, Toshinori
Format Journal Article
LanguageEnglish
Published Bristol IOP Publishing 01.02.2024
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ISSN1742-6588
1742-6596
1742-6596
DOI10.1088/1742-6596/2701/1/012059

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Summary:This study attempts to elucidate the conservation errors induced by the implicit time integration method within a multiscale flow. Using the multiplexed Taylor analytical solution as the initial field, three distinct multiscale turbulence fields were formulated, each characterised by different wavenumber attributes. A two-dimensional inviscid flow field, replicated in a computational domain with a side of 2π and subject to periodic boundary conditions, was used to illuminate kinetic energy conservation errors. The implicit time integration method - specifically the second-order accurate Crank-Nicolson method - was compared with explicit methods, such as the second-order accurate Adams-Bashforth and third-order accurate Runge-Kutta methods. The study also examines the differences between the analytical Taylor solution and a random flow field, particularly in their satisfaction of the Navier-Stokes equations and wavenumber composition, while highlighting the need for preliminary analysis for random flow fields prior to validation calculations.
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ISSN:1742-6588
1742-6596
1742-6596
DOI:10.1088/1742-6596/2701/1/012059