FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2891782489> ?p ?o ?g. }

• W2891782489 endingPage "1256" @default.
• W2891782489 startingPage "1242" @default.
• W2891782489 abstract "In this study, the eulerian probability density function approach (EPDF) has been applied to simulate turbulent diffusion flame in a Vitiated Coflow. EPDF is the eulerian method to solve the PDF transport equations with a direct-quadrature-method-of-moments (DQMOM) closure. The PDF transport equation represented by a set of governing equations for the probability of occurrence in any environmental condition and the probability weighted species mass fractions, which are solved in an eulerian solution [1]; it is considered a product of the delta function, in order to model the turbulence–chemistry interaction. Among these advantages are the prediction and the kinetic control of the species such as CO and NOX. Even though the EPDF approach has been improved in recent years, most improvements have been achieved with parametric study in order to investigate the impact of the model accuracy. The main objective of this investigation is the numerical evaluation of the PDF approach accuracy, using different mixing models and turbulence models, to predict the lift-off height, the extinction and ignition of the flame. Another study comparative of eulerian (EPDF) and lagrangian monte-carlo (LPDF) was applied by equivalent physical models and numerical parameters for evaluating the performances of each approach such as precision and computational specification. The chosen mixture model is the IEM (Interaction by Exchange with the Mean) for micro-mixing closure. The number of environment in the eulerian approach EPDF is (2.0). Through the use of a dynamic model for the mixing time-scale, by computing the individual time-scales for the reactive scalars dynamically in each cell during the course of the simulation using the ANSYS-Fluent/MM-INTAS CFD codes and the chemical reaction mechanism injected is GRI mech 2.1. The results such as mixture fraction, temperature, species mass fraction is validated with experimental data and discussed." @default.
• W2891782489 created "2018-09-27" @default.
• W2891782489 creator A5024043226 @default.
• W2891782489 creator A5024760267 @default.
• W2891782489 creator A5032022827 @default.
• W2891782489 creator A5076230907 @default.
• W2891782489 creator A5084224203 @default.
• W2891782489 date "2018-12-01" @default.
• W2891782489 modified "2023-09-26" @default.
• W2891782489 title "RANS modelling of a lifted hydrogen flame using eulerian/lagrangian approaches with transported PDF method" @default.
• W2891782489 cites W1965315655 @default.
• W2891782489 cites W1973837975 @default.
• W2891782489 cites W1979652870 @default.
• W2891782489 cites W1979756656 @default.
• W2891782489 cites W1981401379 @default.
• W2891782489 cites W1982368848 @default.
• W2891782489 cites W1994376567 @default.
• W2891782489 cites W2006728471 @default.
• W2891782489 cites W2008125897 @default.
• W2891782489 cites W2018984638 @default.
• W2891782489 cites W2024206092 @default.
• W2891782489 cites W2031954861 @default.
• W2891782489 cites W2034361828 @default.
• W2891782489 cites W2039162495 @default.
• W2891782489 cites W2043352533 @default.
• W2891782489 cites W2043575864 @default.
• W2891782489 cites W2043685001 @default.
• W2891782489 cites W2049190161 @default.
• W2891782489 cites W2051438065 @default.
• W2891782489 cites W2058430988 @default.
• W2891782489 cites W2058751371 @default.
• W2891782489 cites W2059018190 @default.
• W2891782489 cites W2064502136 @default.
• W2891782489 cites W2067503648 @default.
• W2891782489 cites W2070419482 @default.
• W2891782489 cites W2076270811 @default.
• W2891782489 cites W2081960346 @default.
• W2891782489 cites W2083685963 @default.
• W2891782489 cites W2084388913 @default.
• W2891782489 cites W2089404277 @default.
• W2891782489 cites W2127061564 @default.
• W2891782489 cites W2133662770 @default.
• W2891782489 cites W2142652554 @default.
• W2891782489 cites W2151729424 @default.
• W2891782489 cites W2164403010 @default.
• W2891782489 cites W2169899461 @default.
• W2891782489 cites W2169944043 @default.
• W2891782489 cites W2587119965 @default.
• W2891782489 cites W2604148858 @default.
• W2891782489 cites W2621311169 @default.
• W2891782489 cites W2796433984 @default.
• W2891782489 doi "https://doi.org/10.1016/j.energy.2018.08.073" @default.
• W2891782489 hasPublicationYear "2018" @default.
• W2891782489 type Work @default.
• W2891782489 sameAs 2891782489 @default.
• W2891782489 citedByCount "5" @default.
• W2891782489 countsByYear W28917824892019 @default.
• W2891782489 countsByYear W28917824892020 @default.
• W2891782489 countsByYear W28917824892021 @default.
• W2891782489 countsByYear W28917824892023 @default.
• W2891782489 crossrefType "journal-article" @default.
• W2891782489 hasAuthorship W2891782489A5024043226 @default.
• W2891782489 hasAuthorship W2891782489A5024760267 @default.
• W2891782489 hasAuthorship W2891782489A5032022827 @default.
• W2891782489 hasAuthorship W2891782489A5076230907 @default.
• W2891782489 hasAuthorship W2891782489A5084224203 @default.
• W2891782489 hasConcept C105795698 @default.
• W2891782489 hasConcept C121332964 @default.
• W2891782489 hasConcept C121864883 @default.
• W2891782489 hasConcept C124101348 @default.
• W2891782489 hasConcept C139002025 @default.
• W2891782489 hasConcept C1633027 @default.
• W2891782489 hasConcept C17456955 @default.
• W2891782489 hasConcept C19499675 @default.
• W2891782489 hasConcept C196558001 @default.
• W2891782489 hasConcept C197055811 @default.
• W2891782489 hasConcept C2778513689 @default.
• W2891782489 hasConcept C28826006 @default.
• W2891782489 hasConcept C32526432 @default.
• W2891782489 hasConcept C33923547 @default.
• W2891782489 hasConcept C41008148 @default.
• W2891782489 hasConcept C43058520 @default.
• W2891782489 hasConcept C53469067 @default.
• W2891782489 hasConcept C57879066 @default.
• W2891782489 hasConceptScore W2891782489C105795698 @default.
• W2891782489 hasConceptScore W2891782489C121332964 @default.
• W2891782489 hasConceptScore W2891782489C121864883 @default.
• W2891782489 hasConceptScore W2891782489C124101348 @default.
• W2891782489 hasConceptScore W2891782489C139002025 @default.
• W2891782489 hasConceptScore W2891782489C1633027 @default.
• W2891782489 hasConceptScore W2891782489C17456955 @default.
• W2891782489 hasConceptScore W2891782489C19499675 @default.
• W2891782489 hasConceptScore W2891782489C196558001 @default.
• W2891782489 hasConceptScore W2891782489C197055811 @default.
• W2891782489 hasConceptScore W2891782489C2778513689 @default.
• W2891782489 hasConceptScore W2891782489C28826006 @default.
• W2891782489 hasConceptScore W2891782489C32526432 @default.
• W2891782489 hasConceptScore W2891782489C33923547 @default.

• next