Matches in SemOpenAlex for { <https://semopenalex.org/work/W2891415427> ?p ?o ?g. }
- W2891415427 endingPage "100" @default.
- W2891415427 startingPage "86" @default.
- W2891415427 abstract "In this study, we assessed the performance of five shock-capturing-type reconstruction schemes in modeling shallow water waves implemented in the public-domain Boussinesq model, FUNWAVE-TVD. The five shock-capturing schemes include two fourth-order Monotonic Upwind Scheme for Conservation Laws - Total Variation Diminishing (MUSCL-TVD) schemes with the Minimod and van-Leer limiters, respectively, a second-order MUSCL-TVD scheme with the van-Leer limiter, a fifth-order Weighted Essentially Non-Oscillatory (WENO) scheme, and a third-order Multi-dimensional Limiting Process (MLP) scheme. Numerical simulations on solitary waves and laboratory measurements showed that for one-dimensional simulations all five shock-capturing schemes maintain non-oscillatory properties, but exhibit different numerical dissipations. Numerical dissipation can be affected by both the order of shock-capturing schemes and choice of limiters. The van-Leer limiter is more dissipative than Minimod when used in fourth-order schemes, which is different from what would be inferred from the linear analysis for the second order. For two-dimensional problems, the shock-capturing schemes can generate either fewer or more high-frequency oscillations, depending on the applied Courant–Friedrichs–Lewy (CFL) number. The most stable results occur in the second-order MUSCL-TVD scheme with the van-Leer limiter, which has large numerical dissipation, and the third-order MLP scheme, which has the ability to control the oscillations in multi-dimensional simulations. The wavelet analysis showed that high-frequency oscillations usually occur at later time and thus affect long-time simulation. Decreasing the CFL number is an effective way of reducing high-frequency oscillations in two-dimensional applications. Models with different shock-capturing schemes can predict similar strength and patterns of wave-induced currents in the breaking wave application. However, the analysis based on the vorticity or enstrophy (integral of the square of the vorticity) calculations show that the schemes with higher numerical dissipation have more significant damping effect on the vorticity field, which may affect the model accuracy in predicting wave-current interaction in a long time simulation." @default.
- W2891415427 created "2018-09-27" @default.
- W2891415427 creator A5009240399 @default.
- W2891415427 creator A5024650901 @default.
- W2891415427 creator A5044401439 @default.
- W2891415427 creator A5087668255 @default.
- W2891415427 date "2018-11-01" @default.
- W2891415427 modified "2023-09-26" @default.
- W2891415427 title "Performance of various shock-capturing-type reconstruction schemes in the Boussinesq wave model, FUNWAVE-TVD" @default.
- W2891415427 cites W1968241756 @default.
- W2891415427 cites W1969647398 @default.
- W2891415427 cites W1970529458 @default.
- W2891415427 cites W1978806404 @default.
- W2891415427 cites W1984246786 @default.
- W2891415427 cites W1989891199 @default.
- W2891415427 cites W1991230420 @default.
- W2891415427 cites W1996468798 @default.
- W2891415427 cites W1997263658 @default.
- W2891415427 cites W1998830482 @default.
- W2891415427 cites W1998980423 @default.
- W2891415427 cites W2006385603 @default.
- W2891415427 cites W2006623593 @default.
- W2891415427 cites W2006976276 @default.
- W2891415427 cites W2010406593 @default.
- W2891415427 cites W2023553466 @default.
- W2891415427 cites W2036738806 @default.
- W2891415427 cites W2037019252 @default.
- W2891415427 cites W2037093232 @default.
- W2891415427 cites W2038435678 @default.
- W2891415427 cites W2039150507 @default.
- W2891415427 cites W2049514147 @default.
- W2891415427 cites W2053711981 @default.
- W2891415427 cites W2053752148 @default.
- W2891415427 cites W2056636248 @default.
- W2891415427 cites W2060802104 @default.
- W2891415427 cites W2067304081 @default.
- W2891415427 cites W2069250702 @default.
- W2891415427 cites W2070394521 @default.
- W2891415427 cites W2078363938 @default.
- W2891415427 cites W2081865159 @default.
- W2891415427 cites W2083085508 @default.
- W2891415427 cites W2083850718 @default.
- W2891415427 cites W2109826025 @default.
- W2891415427 cites W2111286455 @default.
- W2891415427 cites W2114123929 @default.
- W2891415427 cites W2147480329 @default.
- W2891415427 cites W2161529257 @default.
- W2891415427 cites W2166872497 @default.
- W2891415427 cites W2414031430 @default.
- W2891415427 cites W2486793582 @default.
- W2891415427 cites W2514764990 @default.
- W2891415427 cites W2604414411 @default.
- W2891415427 cites W2606671221 @default.
- W2891415427 cites W2768789766 @default.
- W2891415427 doi "https://doi.org/10.1016/j.ocemod.2018.09.004" @default.
- W2891415427 hasPublicationYear "2018" @default.
- W2891415427 type Work @default.
- W2891415427 sameAs 2891415427 @default.
- W2891415427 citedByCount "19" @default.
- W2891415427 countsByYear W28914154272019 @default.
- W2891415427 countsByYear W28914154272020 @default.
- W2891415427 countsByYear W28914154272021 @default.
- W2891415427 countsByYear W28914154272022 @default.
- W2891415427 countsByYear W28914154272023 @default.
- W2891415427 crossrefType "journal-article" @default.
- W2891415427 hasAuthorship W2891415427A5009240399 @default.
- W2891415427 hasAuthorship W2891415427A5024650901 @default.
- W2891415427 hasAuthorship W2891415427A5044401439 @default.
- W2891415427 hasAuthorship W2891415427A5087668255 @default.
- W2891415427 hasConcept C10819784 @default.
- W2891415427 hasConcept C121332964 @default.
- W2891415427 hasConcept C126322002 @default.
- W2891415427 hasConcept C134306372 @default.
- W2891415427 hasConcept C135402231 @default.
- W2891415427 hasConcept C152284280 @default.
- W2891415427 hasConcept C2781300812 @default.
- W2891415427 hasConcept C28826006 @default.
- W2891415427 hasConcept C30295242 @default.
- W2891415427 hasConcept C33923547 @default.
- W2891415427 hasConcept C3445786 @default.
- W2891415427 hasConcept C41008148 @default.
- W2891415427 hasConcept C45011657 @default.
- W2891415427 hasConcept C500300565 @default.
- W2891415427 hasConcept C57879066 @default.
- W2891415427 hasConcept C62520636 @default.
- W2891415427 hasConcept C70477161 @default.
- W2891415427 hasConcept C71924100 @default.
- W2891415427 hasConcept C73000952 @default.
- W2891415427 hasConcept C76155785 @default.
- W2891415427 hasConcept C94025248 @default.
- W2891415427 hasConcept C97355855 @default.
- W2891415427 hasConcept C99692599 @default.
- W2891415427 hasConceptScore W2891415427C10819784 @default.
- W2891415427 hasConceptScore W2891415427C121332964 @default.
- W2891415427 hasConceptScore W2891415427C126322002 @default.
- W2891415427 hasConceptScore W2891415427C134306372 @default.
- W2891415427 hasConceptScore W2891415427C135402231 @default.
- W2891415427 hasConceptScore W2891415427C152284280 @default.