Matches in SemOpenAlex for { <https://semopenalex.org/work/W4292314568> ?p ?o ?g. }
- W4292314568 endingPage "765" @default.
- W4292314568 startingPage "755" @default.
- W4292314568 abstract "With the rapid growth in defense and civilian industry interests, high-performance materials like lattice materials capable of resisting high strain-rate loads are urgently required. Researchers mainly focus on the irreversible plastic deformation of lattice core sandwich structures under out-of-plane loads, whereas the potential application of cellular core without sandwiched face sheets has not been explored. In fact, when shock waves directly act on a cellular core without sandwiched face sheet, the energy would be consumed in the voids during the wave propagation. This article gives an insight into the shock wave attenuation characteristics and the attenuation mechanisms of square cross-sectional truss based meso-scale lattice architectures. Two types of lattice configurations with the same porosity but different truss sectional arrangements are employed. It is reported that both types of the lattice architectures can considerably dissipate the shock wave. The variation trends of overpressure-time history for the meso-scale lattice architectures are significantly different from those obtained in the free air field. As the truss-sectional size decreases the detected first peak overpressure decreases and becomes gradually lower than the second peak overpressure due to the increasing truss layers. When the edge length of truss section, d, decreases from 0.4 mm to 0.1 mm at a constant scaled distance of 0.896, the attenuation efficiency of the peak overpressure is increased by 30 % to 70 %, and the efficiency of the impulse is increased by 60 %, together with a highly-improved increasing rate for the delaying efficiency of the arrival time. Considering distinct scaled distances, the type II architecture and type I architecture behave superiorly with respect to the attenuation efficiencies of peak overpressure and impulse, respectively. Compared to the free field scenario, a shorter wave propagation distance could be observed for the meso-scale lattice architectures to achieve the same peak overpressure and impulse. The considerable shock wave attenuation of the meso-scale lattice architecture is attributed to the complex interactions of the shock wave reflection, diffraction, and superposition around the truss sections and in the voids. This investigation provides a novel method for the shock wave attenuation and energy consumption to protect vital targets and precise equipment." @default.
- W4292314568 created "2022-08-19" @default.
- W4292314568 creator A5005283900 @default.
- W4292314568 creator A5007942235 @default.
- W4292314568 creator A5017435748 @default.
- W4292314568 creator A5019819055 @default.
- W4292314568 date "2022-10-01" @default.
- W4292314568 modified "2023-09-25" @default.
- W4292314568 title "Blast shock wave attenuation in square cross-sectional truss based meso-scale lattice architectures" @default.
- W4292314568 cites W1980227559 @default.
- W4292314568 cites W2003976424 @default.
- W4292314568 cites W2007260551 @default.
- W4292314568 cites W2024143547 @default.
- W4292314568 cites W2031322002 @default.
- W4292314568 cites W2035670660 @default.
- W4292314568 cites W2064390636 @default.
- W4292314568 cites W2064515075 @default.
- W4292314568 cites W2143150831 @default.
- W4292314568 cites W2167983698 @default.
- W4292314568 cites W2342362794 @default.
- W4292314568 cites W2513745894 @default.
- W4292314568 cites W2606096058 @default.
- W4292314568 cites W2795373522 @default.
- W4292314568 cites W2796665879 @default.
- W4292314568 cites W2980635280 @default.
- W4292314568 cites W3008326918 @default.
- W4292314568 cites W3037272318 @default.
- W4292314568 cites W3087021750 @default.
- W4292314568 cites W3087739327 @default.
- W4292314568 cites W3119254886 @default.
- W4292314568 cites W3153015357 @default.
- W4292314568 cites W4200200543 @default.
- W4292314568 cites W4210654011 @default.
- W4292314568 doi "https://doi.org/10.1016/j.istruc.2022.08.020" @default.
- W4292314568 hasPublicationYear "2022" @default.
- W4292314568 type Work @default.
- W4292314568 citedByCount "0" @default.
- W4292314568 crossrefType "journal-article" @default.
- W4292314568 hasAuthorship W4292314568A5005283900 @default.
- W4292314568 hasAuthorship W4292314568A5007942235 @default.
- W4292314568 hasAuthorship W4292314568A5017435748 @default.
- W4292314568 hasAuthorship W4292314568A5019819055 @default.
- W4292314568 hasConcept C120665830 @default.
- W4292314568 hasConcept C121332964 @default.
- W4292314568 hasConcept C127413603 @default.
- W4292314568 hasConcept C159985019 @default.
- W4292314568 hasConcept C173534245 @default.
- W4292314568 hasConcept C184652730 @default.
- W4292314568 hasConcept C192562407 @default.
- W4292314568 hasConcept C24890656 @default.
- W4292314568 hasConcept C26873012 @default.
- W4292314568 hasConcept C2777620828 @default.
- W4292314568 hasConcept C2781204021 @default.
- W4292314568 hasConcept C29452850 @default.
- W4292314568 hasConcept C51329190 @default.
- W4292314568 hasConcept C57879066 @default.
- W4292314568 hasConcept C62520636 @default.
- W4292314568 hasConcept C6648577 @default.
- W4292314568 hasConcept C66938386 @default.
- W4292314568 hasConcept C70477161 @default.
- W4292314568 hasConcept C70836080 @default.
- W4292314568 hasConcept C97355855 @default.
- W4292314568 hasConceptScore W4292314568C120665830 @default.
- W4292314568 hasConceptScore W4292314568C121332964 @default.
- W4292314568 hasConceptScore W4292314568C127413603 @default.
- W4292314568 hasConceptScore W4292314568C159985019 @default.
- W4292314568 hasConceptScore W4292314568C173534245 @default.
- W4292314568 hasConceptScore W4292314568C184652730 @default.
- W4292314568 hasConceptScore W4292314568C192562407 @default.
- W4292314568 hasConceptScore W4292314568C24890656 @default.
- W4292314568 hasConceptScore W4292314568C26873012 @default.
- W4292314568 hasConceptScore W4292314568C2777620828 @default.
- W4292314568 hasConceptScore W4292314568C2781204021 @default.
- W4292314568 hasConceptScore W4292314568C29452850 @default.
- W4292314568 hasConceptScore W4292314568C51329190 @default.
- W4292314568 hasConceptScore W4292314568C57879066 @default.
- W4292314568 hasConceptScore W4292314568C62520636 @default.
- W4292314568 hasConceptScore W4292314568C6648577 @default.
- W4292314568 hasConceptScore W4292314568C66938386 @default.
- W4292314568 hasConceptScore W4292314568C70477161 @default.
- W4292314568 hasConceptScore W4292314568C70836080 @default.
- W4292314568 hasConceptScore W4292314568C97355855 @default.
- W4292314568 hasFunder F4320321001 @default.
- W4292314568 hasLocation W42923145681 @default.
- W4292314568 hasOpenAccess W4292314568 @default.
- W4292314568 hasPrimaryLocation W42923145681 @default.
- W4292314568 hasRelatedWork W1975047948 @default.
- W4292314568 hasRelatedWork W1991493249 @default.
- W4292314568 hasRelatedWork W2075580692 @default.
- W4292314568 hasRelatedWork W2076160155 @default.
- W4292314568 hasRelatedWork W2093275523 @default.
- W4292314568 hasRelatedWork W2348937202 @default.
- W4292314568 hasRelatedWork W2373584518 @default.
- W4292314568 hasRelatedWork W2384279159 @default.
- W4292314568 hasRelatedWork W2974074585 @default.
- W4292314568 hasRelatedWork W4200154337 @default.
- W4292314568 hasVolume "44" @default.
- W4292314568 isParatext "false" @default.