Matches in SemOpenAlex for { <https://semopenalex.org/work/W2023605818> ?p ?o ?g. }
- W2023605818 endingPage "822" @default.
- W2023605818 startingPage "781" @default.
- W2023605818 abstract "Heterogeneous high-energy explosives are morphologically, mechanically and chemically complex. As such, their ab initio modelling, in which well-characterized phenomena at the scale of the microstructure lead to a rationally homogenized description at the much larger scale of observation, is a subject of active research but not yet a reality. An alternative approach is to construct phenomenological models, in which forms of constitutive behaviour are postulated with an eye on the perceived picture of the micro-scale phenomena, and which are strongly linked to experimental calibration. Most prominent among these is the ignition-and-growth model conceived by Lee and Tarver. The model treats the explosive as a homogeneous mixture of two distinct constituents, the unreacted explosive and the products of reaction. To each constituent is assigned an equation of state, and a single reaction-rate law is prescribed for the conversion of the explosive to products. It is assumed that the two constituents are always in pressure and temperature equilibrium. The purpose of this paper is to investigate in detail the behaviour of the model in situations where a detonation turns a corner and undergoes diffraction. A set of parameters appropriate for the explosive LX-17 is selected. The model is first examined analytically for steady, planar, one-dimensional (1D) solutions and the reaction-zone structure of Chapman–Jouguet detonations is determined. A computational study of two classes of problems is then undertaken. The first class corresponds to planar, 1D initiation by an impact, and the second to corner turning and diffraction in planar and axisymmetric geometries. The 1D initiation, although interesting in its own right, is utilized here as a means for interpretation of the two-dimensional results. It is found that there are two generic ways in which 1D detonations are initiated in the model, and that these scenarios play a part in the post-diffraction evolution as well. For the parameter set under study the model shows detonation failure, but only locally and temporarily, and does not generate sustained dead zones. The computations employ adaptive mesh refinement and are finely resolved. Results are obtained for a rigid confinement of the explosive. Compliant confinement represents its own computational challenges and is currently under study. Also under development is an extended ignition-and-growth model which takes into account observed desensitization of heterogeneous explosives by weak shocks." @default.
- W2023605818 created "2016-06-24" @default.
- W2023605818 creator A5009318563 @default.
- W2023605818 creator A5058192332 @default.
- W2023605818 creator A5069419886 @default.
- W2023605818 creator A5072477813 @default.
- W2023605818 date "2007-09-18" @default.
- W2023605818 modified "2023-09-24" @default.
- W2023605818 title "A study of detonation diffraction in the ignition-and-growth model" @default.
- W2023605818 cites W1489356445 @default.
- W2023605818 cites W1512062588 @default.
- W2023605818 cites W1975059575 @default.
- W2023605818 cites W1976845298 @default.
- W2023605818 cites W1990653832 @default.
- W2023605818 cites W2015512134 @default.
- W2023605818 cites W2026307951 @default.
- W2023605818 cites W2052876220 @default.
- W2023605818 cites W2056307165 @default.
- W2023605818 cites W2064101210 @default.
- W2023605818 cites W2086644435 @default.
- W2023605818 cites W2117778416 @default.
- W2023605818 cites W2152830908 @default.
- W2023605818 cites W2252820167 @default.
- W2023605818 cites W4245037559 @default.
- W2023605818 cites W4382891143 @default.
- W2023605818 doi "https://doi.org/10.1080/13647830701235774" @default.
- W2023605818 hasPublicationYear "2007" @default.
- W2023605818 type Work @default.
- W2023605818 sameAs 2023605818 @default.
- W2023605818 citedByCount "50" @default.
- W2023605818 countsByYear W20236058182012 @default.
- W2023605818 countsByYear W20236058182013 @default.
- W2023605818 countsByYear W20236058182014 @default.
- W2023605818 countsByYear W20236058182015 @default.
- W2023605818 countsByYear W20236058182016 @default.
- W2023605818 countsByYear W20236058182017 @default.
- W2023605818 countsByYear W20236058182018 @default.
- W2023605818 countsByYear W20236058182019 @default.
- W2023605818 countsByYear W20236058182020 @default.
- W2023605818 countsByYear W20236058182021 @default.
- W2023605818 countsByYear W20236058182022 @default.
- W2023605818 crossrefType "journal-article" @default.
- W2023605818 hasAuthorship W2023605818A5009318563 @default.
- W2023605818 hasAuthorship W2023605818A5058192332 @default.
- W2023605818 hasAuthorship W2023605818A5069419886 @default.
- W2023605818 hasAuthorship W2023605818A5072477813 @default.
- W2023605818 hasBestOaLocation W20236058182 @default.
- W2023605818 hasConcept C11135259 @default.
- W2023605818 hasConcept C120665830 @default.
- W2023605818 hasConcept C121332964 @default.
- W2023605818 hasConcept C121684516 @default.
- W2023605818 hasConcept C121864883 @default.
- W2023605818 hasConcept C134786449 @default.
- W2023605818 hasConcept C154238967 @default.
- W2023605818 hasConcept C159063594 @default.
- W2023605818 hasConcept C178790620 @default.
- W2023605818 hasConcept C185592680 @default.
- W2023605818 hasConcept C192562407 @default.
- W2023605818 hasConcept C203397868 @default.
- W2023605818 hasConcept C207114421 @default.
- W2023605818 hasConcept C2777009965 @default.
- W2023605818 hasConcept C2778755073 @default.
- W2023605818 hasConcept C2779569378 @default.
- W2023605818 hasConcept C2781442258 @default.
- W2023605818 hasConcept C41008148 @default.
- W2023605818 hasConcept C57879066 @default.
- W2023605818 hasConcept C62520636 @default.
- W2023605818 hasConcept C66882249 @default.
- W2023605818 hasConcept C97355855 @default.
- W2023605818 hasConceptScore W2023605818C11135259 @default.
- W2023605818 hasConceptScore W2023605818C120665830 @default.
- W2023605818 hasConceptScore W2023605818C121332964 @default.
- W2023605818 hasConceptScore W2023605818C121684516 @default.
- W2023605818 hasConceptScore W2023605818C121864883 @default.
- W2023605818 hasConceptScore W2023605818C134786449 @default.
- W2023605818 hasConceptScore W2023605818C154238967 @default.
- W2023605818 hasConceptScore W2023605818C159063594 @default.
- W2023605818 hasConceptScore W2023605818C178790620 @default.
- W2023605818 hasConceptScore W2023605818C185592680 @default.
- W2023605818 hasConceptScore W2023605818C192562407 @default.
- W2023605818 hasConceptScore W2023605818C203397868 @default.
- W2023605818 hasConceptScore W2023605818C207114421 @default.
- W2023605818 hasConceptScore W2023605818C2777009965 @default.
- W2023605818 hasConceptScore W2023605818C2778755073 @default.
- W2023605818 hasConceptScore W2023605818C2779569378 @default.
- W2023605818 hasConceptScore W2023605818C2781442258 @default.
- W2023605818 hasConceptScore W2023605818C41008148 @default.
- W2023605818 hasConceptScore W2023605818C57879066 @default.
- W2023605818 hasConceptScore W2023605818C62520636 @default.
- W2023605818 hasConceptScore W2023605818C66882249 @default.
- W2023605818 hasConceptScore W2023605818C97355855 @default.
- W2023605818 hasIssue "5" @default.
- W2023605818 hasLocation W20236058181 @default.
- W2023605818 hasLocation W20236058182 @default.
- W2023605818 hasLocation W20236058183 @default.
- W2023605818 hasOpenAccess W2023605818 @default.
- W2023605818 hasPrimaryLocation W20236058181 @default.
- W2023605818 hasRelatedWork W1971259425 @default.