Matches in SemOpenAlex for { <https://semopenalex.org/work/W4311551485> ?p ?o ?g. }
- W4311551485 endingPage "112560" @default.
- W4311551485 startingPage "112560" @default.
- W4311551485 abstract "Combustion of hydrogen can help in reducing carbon-based emissions but it also poses unique challenges related to the high flame speed and Lewis number effects of the hydrogen flame. When operated with conventional burners, a hydrogen flame can flashback at higher volumetric flow rates than a methane flame due to the difference in stabilization mechanisms of the two fuels. Due to these differences, conventional burners cannot offer similar operational ranges for hydrogen than that for hydrocarbon flames. An exploration into the unique stabilization behaviour of hydrogen flames is required which could help in envisioning non-conventional burner concepts for keeping hydrogen flames stable. Stability conditions, which describe the kinematics of premixed flames with spatially and temporally changing flow parameters, are crucial for such an exploration. Stability conditions are usually hypothesized for stable flames, where a flame upon perturbation is assumed to return to its original position. Alternatively, in the case of flashback/blow-off, it refers to a flame moving upstream of the burner or being convected out of the domain. However, it is also of interest to understand how and why a flame could move to a new location when the velocity and strain fields are varying with time and space at the original and the new location. In this paper, we investigate the flame stabilization by 1) observing the hydrogen flame’s upstream movement in a multi-slit configuration when a geometrical change is made, and 2) changing strain and velocity fields in a dynamic and periodic manner using numerical tools such that the unique behaviour of a hydrogen flame can be captured. We vary the location of high flow strain periodically in a channel by manipulating the boundary condition along a wall. It is found that a hydrogen flame follows this point in a periodic manner, also propagating against the inflow which is considerably faster than its unstretched burning velocity. Spatial and temporal stability conditions, that explain the mechanism behind the flame’s movement from its original position to a new position, are analyzed from the simulation data, advancing our knowledge on the flame movement in an unsteady setting and providing important insights into the stabilization mechanism of hydrogen flames." @default.
- W4311551485 created "2022-12-27" @default.
- W4311551485 creator A5002293047 @default.
- W4311551485 creator A5030322036 @default.
- W4311551485 creator A5034190951 @default.
- W4311551485 creator A5066728861 @default.
- W4311551485 creator A5071818658 @default.
- W4311551485 date "2023-02-01" @default.
- W4311551485 modified "2023-10-03" @default.
- W4311551485 title "Dynamic stabilization of a hydrogen premixed flame in a narrow channel" @default.
- W4311551485 cites W1027777258 @default.
- W4311551485 cites W1967575856 @default.
- W4311551485 cites W1990323035 @default.
- W4311551485 cites W1991074315 @default.
- W4311551485 cites W2030165098 @default.
- W4311551485 cites W2033903721 @default.
- W4311551485 cites W2039758898 @default.
- W4311551485 cites W2055356626 @default.
- W4311551485 cites W2086780989 @default.
- W4311551485 cites W2143831171 @default.
- W4311551485 cites W2150667450 @default.
- W4311551485 cites W2151678193 @default.
- W4311551485 cites W2151791361 @default.
- W4311551485 cites W2186014971 @default.
- W4311551485 cites W2412528273 @default.
- W4311551485 cites W2476493996 @default.
- W4311551485 cites W2530245997 @default.
- W4311551485 cites W2543417560 @default.
- W4311551485 cites W2549095134 @default.
- W4311551485 cites W2549680589 @default.
- W4311551485 cites W2765075687 @default.
- W4311551485 cites W2783607095 @default.
- W4311551485 cites W2787999240 @default.
- W4311551485 cites W2808851615 @default.
- W4311551485 cites W2883009774 @default.
- W4311551485 cites W2885727050 @default.
- W4311551485 cites W2903289765 @default.
- W4311551485 cites W2913454984 @default.
- W4311551485 cites W2959750456 @default.
- W4311551485 cites W2984302784 @default.
- W4311551485 cites W2997573140 @default.
- W4311551485 cites W3009715488 @default.
- W4311551485 cites W3013769237 @default.
- W4311551485 cites W3032945115 @default.
- W4311551485 cites W3045151286 @default.
- W4311551485 cites W3046649064 @default.
- W4311551485 cites W3086060716 @default.
- W4311551485 cites W3092360653 @default.
- W4311551485 cites W3094931093 @default.
- W4311551485 cites W3141177090 @default.
- W4311551485 cites W3195199205 @default.
- W4311551485 cites W3200354245 @default.
- W4311551485 cites W4200231390 @default.
- W4311551485 cites W4213176171 @default.
- W4311551485 cites W4280609252 @default.
- W4311551485 doi "https://doi.org/10.1016/j.combustflame.2022.112560" @default.
- W4311551485 hasPublicationYear "2023" @default.
- W4311551485 type Work @default.
- W4311551485 citedByCount "1" @default.
- W4311551485 countsByYear W43115514852023 @default.
- W4311551485 crossrefType "journal-article" @default.
- W4311551485 hasAuthorship W4311551485A5002293047 @default.
- W4311551485 hasAuthorship W4311551485A5030322036 @default.
- W4311551485 hasAuthorship W4311551485A5034190951 @default.
- W4311551485 hasAuthorship W4311551485A5066728861 @default.
- W4311551485 hasAuthorship W4311551485A5071818658 @default.
- W4311551485 hasConcept C105923489 @default.
- W4311551485 hasConcept C121332964 @default.
- W4311551485 hasConcept C129474609 @default.
- W4311551485 hasConcept C178790620 @default.
- W4311551485 hasConcept C185592680 @default.
- W4311551485 hasConcept C207870545 @default.
- W4311551485 hasConcept C2778269189 @default.
- W4311551485 hasConcept C2778560903 @default.
- W4311551485 hasConcept C512968161 @default.
- W4311551485 hasConcept C516920438 @default.
- W4311551485 hasConcept C55477048 @default.
- W4311551485 hasConcept C57879066 @default.
- W4311551485 hasConcept C6506403 @default.
- W4311551485 hasConcept C7742248 @default.
- W4311551485 hasConcept C83104080 @default.
- W4311551485 hasConceptScore W4311551485C105923489 @default.
- W4311551485 hasConceptScore W4311551485C121332964 @default.
- W4311551485 hasConceptScore W4311551485C129474609 @default.
- W4311551485 hasConceptScore W4311551485C178790620 @default.
- W4311551485 hasConceptScore W4311551485C185592680 @default.
- W4311551485 hasConceptScore W4311551485C207870545 @default.
- W4311551485 hasConceptScore W4311551485C2778269189 @default.
- W4311551485 hasConceptScore W4311551485C2778560903 @default.
- W4311551485 hasConceptScore W4311551485C512968161 @default.
- W4311551485 hasConceptScore W4311551485C516920438 @default.
- W4311551485 hasConceptScore W4311551485C55477048 @default.
- W4311551485 hasConceptScore W4311551485C57879066 @default.
- W4311551485 hasConceptScore W4311551485C6506403 @default.
- W4311551485 hasConceptScore W4311551485C7742248 @default.
- W4311551485 hasConceptScore W4311551485C83104080 @default.
- W4311551485 hasLocation W43115514851 @default.
- W4311551485 hasOpenAccess W4311551485 @default.