Matches in SemOpenAlex for { <https://semopenalex.org/work/W2085996766> ?p ?o ?g. }
- W2085996766 endingPage "6664" @default.
- W2085996766 startingPage "6643" @default.
- W2085996766 abstract "There is great difficulty for direct Boltzmann solvers to simulate high Knudsen number flow due to the severe steep slope and high concentration of the gas distribution function in a local particle velocity space. Local mesh adaptation becomes necessary in order to make the Boltzmann solver to be a practical tool in aerospace applications. The present research improves the unified gas-kinetic scheme (UGKS) in the following two aspects. First, the UGKS is extended in a physical space with moving mesh. This technique is important to study a freely flying object in a rarefied environment. Second, the adaptive quadtree method in the particle velocity space is implemented in the UGKS. Due to the new improvements in the discretization of a gas distribution function in the six dimensional phase space, the adaptive unified gas kinetic scheme (AUGKS) is able to deal with a wide range of flow problems under extreme flying conditions, such as the whole unsteady flying process of an object from a highly rarefied to a continuum flow regime. After validating the scheme, the capability of AUGKS is demonstrated in the following two challenge test cases. The first case is about the free movement of an ellipse flying at initial Mach number 5 in a rarefied flow at different Knudsen numbers. The force on the ellipse and the unsteady trajectory of the ellipse movement are fully captured. The gas distribution function around the ellipse is analyzed. The second case is about the study of unsteady flight of a nozzle under a bursting process of the compressed gas expanding into a rarefied environment. Due to the strong expansion wave and the huge density difference between interior and exterior regions around the nozzle, the particle distribution function changes dramatically in the particle velocity space. The use of an adaptive velocity space in the AUGKS becomes necessary to simulate such a flow and to control the computational cost to a tolerable level. The second test is a challenge problem for any existing rarefied flow solver." @default.
- W2085996766 created "2016-06-24" @default.
- W2085996766 creator A5038382239 @default.
- W2085996766 creator A5050401971 @default.
- W2085996766 creator A5052037068 @default.
- W2085996766 creator A5059193287 @default.
- W2085996766 date "2012-08-01" @default.
- W2085996766 modified "2023-10-14" @default.
- W2085996766 title "A unified gas kinetic scheme with moving mesh and velocity space adaptation" @default.
- W2085996766 cites W1969830762 @default.
- W2085996766 cites W1975734689 @default.
- W2085996766 cites W1982393680 @default.
- W2085996766 cites W1986752469 @default.
- W2085996766 cites W2001364727 @default.
- W2085996766 cites W2006016817 @default.
- W2085996766 cites W2006450963 @default.
- W2085996766 cites W2013702974 @default.
- W2085996766 cites W2017700359 @default.
- W2085996766 cites W2019418641 @default.
- W2085996766 cites W2033939545 @default.
- W2085996766 cites W2038814417 @default.
- W2085996766 cites W2041043435 @default.
- W2085996766 cites W2047242919 @default.
- W2085996766 cites W2049849994 @default.
- W2085996766 cites W2056706689 @default.
- W2085996766 cites W2058487438 @default.
- W2085996766 cites W2061374290 @default.
- W2085996766 cites W2061953290 @default.
- W2085996766 cites W2064630706 @default.
- W2085996766 cites W2068102804 @default.
- W2085996766 cites W2074021850 @default.
- W2085996766 cites W2074478842 @default.
- W2085996766 cites W2081439996 @default.
- W2085996766 cites W2085955212 @default.
- W2085996766 cites W2087360755 @default.
- W2085996766 cites W2089355912 @default.
- W2085996766 cites W2100201447 @default.
- W2085996766 cites W2106363470 @default.
- W2085996766 cites W2106743858 @default.
- W2085996766 cites W2108973612 @default.
- W2085996766 cites W2131947874 @default.
- W2085996766 cites W2154670229 @default.
- W2085996766 cites W4251706365 @default.
- W2085996766 doi "https://doi.org/10.1016/j.jcp.2012.05.019" @default.
- W2085996766 hasPublicationYear "2012" @default.
- W2085996766 type Work @default.
- W2085996766 sameAs 2085996766 @default.
- W2085996766 citedByCount "108" @default.
- W2085996766 countsByYear W20859967662012 @default.
- W2085996766 countsByYear W20859967662013 @default.
- W2085996766 countsByYear W20859967662014 @default.
- W2085996766 countsByYear W20859967662015 @default.
- W2085996766 countsByYear W20859967662016 @default.
- W2085996766 countsByYear W20859967662017 @default.
- W2085996766 countsByYear W20859967662018 @default.
- W2085996766 countsByYear W20859967662019 @default.
- W2085996766 countsByYear W20859967662020 @default.
- W2085996766 countsByYear W20859967662021 @default.
- W2085996766 countsByYear W20859967662022 @default.
- W2085996766 countsByYear W20859967662023 @default.
- W2085996766 crossrefType "journal-article" @default.
- W2085996766 hasAuthorship W2085996766A5038382239 @default.
- W2085996766 hasAuthorship W2085996766A5050401971 @default.
- W2085996766 hasAuthorship W2085996766A5052037068 @default.
- W2085996766 hasAuthorship W2085996766A5059193287 @default.
- W2085996766 hasConcept C121332964 @default.
- W2085996766 hasConcept C121838276 @default.
- W2085996766 hasConcept C131053463 @default.
- W2085996766 hasConcept C134306372 @default.
- W2085996766 hasConcept C165231844 @default.
- W2085996766 hasConcept C186603090 @default.
- W2085996766 hasConcept C2524010 @default.
- W2085996766 hasConcept C33923547 @default.
- W2085996766 hasConcept C38349280 @default.
- W2085996766 hasConcept C41008148 @default.
- W2085996766 hasConcept C459310 @default.
- W2085996766 hasConcept C57879066 @default.
- W2085996766 hasConcept C62520636 @default.
- W2085996766 hasConcept C73000952 @default.
- W2085996766 hasConcept C74261601 @default.
- W2085996766 hasConcept C74650414 @default.
- W2085996766 hasConceptScore W2085996766C121332964 @default.
- W2085996766 hasConceptScore W2085996766C121838276 @default.
- W2085996766 hasConceptScore W2085996766C131053463 @default.
- W2085996766 hasConceptScore W2085996766C134306372 @default.
- W2085996766 hasConceptScore W2085996766C165231844 @default.
- W2085996766 hasConceptScore W2085996766C186603090 @default.
- W2085996766 hasConceptScore W2085996766C2524010 @default.
- W2085996766 hasConceptScore W2085996766C33923547 @default.
- W2085996766 hasConceptScore W2085996766C38349280 @default.
- W2085996766 hasConceptScore W2085996766C41008148 @default.
- W2085996766 hasConceptScore W2085996766C459310 @default.
- W2085996766 hasConceptScore W2085996766C57879066 @default.
- W2085996766 hasConceptScore W2085996766C62520636 @default.
- W2085996766 hasConceptScore W2085996766C73000952 @default.
- W2085996766 hasConceptScore W2085996766C74261601 @default.
- W2085996766 hasConceptScore W2085996766C74650414 @default.
- W2085996766 hasFunder F4320321001 @default.