FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2884987672> ?p ?o ?g. }

• W2884987672 endingPage "571" @default.
• W2884987672 startingPage "541" @default.
• W2884987672 abstract "Mixed zig-zag plate theories are derived from a recently developed 3-D five d.o.f. zig-zag “adaptive” theory ZZA (a priori fulfillment of interfacial stress constraints) under steadily growing limiting assumptions on displacement, strain and stress fields. The intended aim is trying to save computational costs simultaneously preserving accuracy. Lower-order theories assume a uniform or a polynomial transverse displacement, out-of-plane stresses are derived from local equilibrium equations or retaken from higher-order theories. The focus of this study is twofold: (i) to assess whether and for which cases a higher-order through-thickness zig-zag transverse displacement representation is essential, or vice versa a simpler kinematics can be assumed; (ii) to compare accuracy of theories based on Murakami's and Di Sciuva's zig-zag functions with the same expansion order across the thickness. A number of challenging benchmarks are retaken from literature and new benchmarks with a strong variation of material properties (damaged layers), distributed or localized step loading and some different boundary conditions are considered to assess accuracy of theories and of FEA 3-D (constituting the reference solution in lack of exact results). For these benchmarks, closed-form solutions are obtained assuming the same expansion order across the thickness and the same in-plane trial functions for all theories. The numerical illustrations show that lower order and Murakami's based theories fail for cases having the strongest layerwise and transverse anisotropy effects, or a marked through-thickness asymmetry. The Hu–Washizu highest-order theory HWZZ is shown to be always the only as accurate as ZZA, despite it reduces the computational effort." @default.
• W2884987672 created "2018-08-03" @default.
• W2884987672 creator A5002752735 @default.
• W2884987672 creator A5079790548 @default.
• W2884987672 date "2018-09-01" @default.
• W2884987672 modified "2023-09-26" @default.
• W2884987672 title "Novel HW mixed zig-zag theory accounting for transverse normal deformability and lower-order counterparts assessed by old and new elastostatic benchmarks" @default.
• W2884987672 cites W1946447890 @default.
• W2884987672 cites W1964984679 @default.
• W2884987672 cites W1976529791 @default.
• W2884987672 cites W1977959209 @default.
• W2884987672 cites W1978683584 @default.
• W2884987672 cites W1985765530 @default.
• W2884987672 cites W1991289302 @default.
• W2884987672 cites W2004536296 @default.
• W2884987672 cites W2013582389 @default.
• W2884987672 cites W2014384504 @default.
• W2884987672 cites W2014450589 @default.
• W2884987672 cites W2016667548 @default.
• W2884987672 cites W2021431918 @default.
• W2884987672 cites W2028600250 @default.
• W2884987672 cites W2029399612 @default.
• W2884987672 cites W2032415697 @default.
• W2884987672 cites W2033347626 @default.
• W2884987672 cites W2034296432 @default.
• W2884987672 cites W2042655683 @default.
• W2884987672 cites W2058543947 @default.
• W2884987672 cites W2058820159 @default.
• W2884987672 cites W2071812669 @default.
• W2884987672 cites W2072446689 @default.
• W2884987672 cites W2075343494 @default.
• W2884987672 cites W2076220025 @default.
• W2884987672 cites W2083119638 @default.
• W2884987672 cites W2083242863 @default.
• W2884987672 cites W2083613253 @default.
• W2884987672 cites W2089006019 @default.
• W2884987672 cites W2093141860 @default.
• W2884987672 cites W2095235725 @default.
• W2884987672 cites W2106664212 @default.
• W2884987672 cites W2112007419 @default.
• W2884987672 cites W2126630147 @default.
• W2884987672 cites W2131345487 @default.
• W2884987672 cites W2140224112 @default.
• W2884987672 cites W2141565407 @default.
• W2884987672 cites W2155315802 @default.
• W2884987672 cites W2162778806 @default.
• W2884987672 cites W2165237945 @default.
• W2884987672 cites W2166384871 @default.
• W2884987672 cites W2299154496 @default.
• W2884987672 cites W2347180468 @default.
• W2884987672 cites W2520275124 @default.
• W2884987672 doi "https://doi.org/10.1016/j.ast.2018.07.040" @default.
• W2884987672 hasPublicationYear "2018" @default.
• W2884987672 type Work @default.
• W2884987672 sameAs 2884987672 @default.
• W2884987672 citedByCount "5" @default.
• W2884987672 countsByYear W28849876722019 @default.
• W2884987672 countsByYear W28849876722020 @default.
• W2884987672 countsByYear W28849876722022 @default.
• W2884987672 countsByYear W28849876722023 @default.
• W2884987672 crossrefType "journal-article" @default.
• W2884987672 hasAuthorship W2884987672A5002752735 @default.
• W2884987672 hasAuthorship W2884987672A5079790548 @default.
• W2884987672 hasConcept C10138342 @default.
• W2884987672 hasConcept C107551265 @default.
• W2884987672 hasConcept C111472728 @default.
• W2884987672 hasConcept C120665830 @default.
• W2884987672 hasConcept C121332964 @default.
• W2884987672 hasConcept C127413603 @default.
• W2884987672 hasConcept C134306372 @default.
• W2884987672 hasConcept C138885662 @default.
• W2884987672 hasConcept C154954056 @default.
• W2884987672 hasConcept C15744967 @default.
• W2884987672 hasConcept C162324750 @default.
• W2884987672 hasConcept C17744445 @default.
• W2884987672 hasConcept C17825722 @default.
• W2884987672 hasConcept C179254644 @default.
• W2884987672 hasConcept C182306322 @default.
• W2884987672 hasConcept C186068551 @default.
• W2884987672 hasConcept C192271897 @default.
• W2884987672 hasConcept C199539241 @default.
• W2884987672 hasConcept C21036866 @default.
• W2884987672 hasConcept C2524010 @default.
• W2884987672 hasConcept C2776359362 @default.
• W2884987672 hasConcept C33923547 @default.
• W2884987672 hasConcept C38976095 @default.
• W2884987672 hasConcept C41895202 @default.
• W2884987672 hasConcept C542102704 @default.
• W2884987672 hasConcept C62354387 @default.
• W2884987672 hasConcept C62520636 @default.
• W2884987672 hasConcept C66938386 @default.
• W2884987672 hasConcept C74650414 @default.
• W2884987672 hasConcept C75553542 @default.
• W2884987672 hasConcept C85725439 @default.
• W2884987672 hasConcept C94625758 @default.
• W2884987672 hasConceptScore W2884987672C10138342 @default.
• W2884987672 hasConceptScore W2884987672C107551265 @default.
• W2884987672 hasConceptScore W2884987672C111472728 @default.

• next