FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W3135468540> ?p ?o ?g. }

• W3135468540 endingPage "13" @default.
• W3135468540 startingPage "1" @default.
• W3135468540 abstract "To examine the influence of radiative transitions on the performance of nonequilibrium seed-free argon plasma magnetohydrodynamic (MHD) generators, we developed MHD numerical simulation technique with a collisional-radiative (C-R) model, where neutral argon atoms with 45 discrete effective electronic excitation levels, singly ionized argon ions, and free electrons were considered under a two-temperature, low-magnetic Reynolds number MHD approximation. Furthermore, a so-called escape factor was implemented in the C-R model to consider the effects of radiation trapping by ground-state neutral atoms. Using the developed technique, we computed the performance characteristics of a nonequilibrium seed-free argon plasma MHD generator. The numerical results showed that the generator performance gets higher as the escape factor decreases, i.e., the optical thickness for radiative transitions to the ground state of neutral atoms increases. The numerical results also suggested that when the escape factor is <inline-formula xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink> <tex-math notation=LaTeX>$1.0times 10^{-3}$ </tex-math></inline-formula> or less, the generator performance is almost the same as that for the escape factor of 0 corresponding to completely optical-thick plasma case for the radiative transitions to the ground state of neutral atoms. Furthermore, realistic escape factor values for resonance lines in the power generation channel were evaluated using a well-known estimation model. Consequently, the estimated values had the order of <inline-formula xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink> <tex-math notation=LaTeX>$10^{-4}$ </tex-math></inline-formula> . We also showed that under such relatively optically thick plasma cases, a collisional (C) model and a widely used global ionization-recombination rate model with no explicit consideration of electronically excited-state neutral atoms can reproduce the generator performance predicted by the C-R model with relatively good accuracy." @default.
• W3135468540 created "2021-03-15" @default.
• W3135468540 creator A5034865570 @default.
• W3135468540 creator A5035781460 @default.
• W3135468540 creator A5057075069 @default.
• W3135468540 date "2021-01-01" @default.
• W3135468540 modified "2023-09-23" @default.
• W3135468540 title "Numerical Study of Nonequilibrium Seed-Free Argon Plasma Magnetohydrodynamic Generator Using Collisional-Radiative Model" @default.
• W3135468540 cites W1538462587 @default.
• W3135468540 cites W1971980555 @default.
• W3135468540 cites W1976701098 @default.
• W3135468540 cites W2002777584 @default.
• W3135468540 cites W2006777792 @default.
• W3135468540 cites W2026186116 @default.
• W3135468540 cites W2026648602 @default.
• W3135468540 cites W2056346512 @default.
• W3135468540 cites W2067573732 @default.
• W3135468540 cites W2070340710 @default.
• W3135468540 cites W2085650367 @default.
• W3135468540 cites W2090439331 @default.
• W3135468540 cites W2099294274 @default.
• W3135468540 cites W2108487254 @default.
• W3135468540 cites W2116243151 @default.
• W3135468540 cites W2118433564 @default.
• W3135468540 cites W2124548644 @default.
• W3135468540 cites W2127325891 @default.
• W3135468540 cites W2318074201 @default.
• W3135468540 cites W2583184873 @default.
• W3135468540 cites W2805940452 @default.
• W3135468540 cites W2099570633 @default.
• W3135468540 doi "https://doi.org/10.1109/tps.2021.3059440" @default.
• W3135468540 hasPublicationYear "2021" @default.
• W3135468540 type Work @default.
• W3135468540 sameAs 3135468540 @default.
• W3135468540 citedByCount "1" @default.
• W3135468540 countsByYear W31354685402022 @default.
• W3135468540 crossrefType "journal-article" @default.
• W3135468540 hasAuthorship W3135468540A5034865570 @default.
• W3135468540 hasAuthorship W3135468540A5035781460 @default.
• W3135468540 hasAuthorship W3135468540A5057075069 @default.
• W3135468540 hasConcept C121332964 @default.
• W3135468540 hasConcept C184779094 @default.
• W3135468540 hasConcept C30475298 @default.
• W3135468540 hasConcept C31532427 @default.
• W3135468540 hasConcept C42471609 @default.
• W3135468540 hasConcept C47462728 @default.
• W3135468540 hasConcept C547737533 @default.
• W3135468540 hasConcept C62520636 @default.
• W3135468540 hasConcept C74902906 @default.
• W3135468540 hasConcept C82706917 @default.
• W3135468540 hasConceptScore W3135468540C121332964 @default.
• W3135468540 hasConceptScore W3135468540C184779094 @default.
• W3135468540 hasConceptScore W3135468540C30475298 @default.
• W3135468540 hasConceptScore W3135468540C31532427 @default.
• W3135468540 hasConceptScore W3135468540C42471609 @default.
• W3135468540 hasConceptScore W3135468540C47462728 @default.
• W3135468540 hasConceptScore W3135468540C547737533 @default.
• W3135468540 hasConceptScore W3135468540C62520636 @default.
• W3135468540 hasConceptScore W3135468540C74902906 @default.
• W3135468540 hasConceptScore W3135468540C82706917 @default.
• W3135468540 hasLocation W31354685401 @default.
• W3135468540 hasOpenAccess W3135468540 @default.
• W3135468540 hasPrimaryLocation W31354685401 @default.
• W3135468540 hasRelatedWork W1977832713 @default.
• W3135468540 hasRelatedWork W2006862793 @default.
• W3135468540 hasRelatedWork W2023912655 @default.
• W3135468540 hasRelatedWork W2030079375 @default.
• W3135468540 hasRelatedWork W2081307237 @default.
• W3135468540 hasRelatedWork W2158945968 @default.
• W3135468540 hasRelatedWork W2405877283 @default.
• W3135468540 hasRelatedWork W2741650948 @default.
• W3135468540 hasRelatedWork W3127495381 @default.
• W3135468540 hasRelatedWork W2184454773 @default.
• W3135468540 isParatext "false" @default.
• W3135468540 isRetracted "false" @default.
• W3135468540 magId "3135468540" @default.
• W3135468540 workType "article" @default.