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    The Underwater Blast Resistance of Metallic Sandwich Beams With Prismatic Lattice Cores

    Source: Journal of Applied Mechanics:;2007:;volume( 074 ):;issue: 002::page 352
    Author:
    G. J. McShane
    ,
    V. S. Deshpande
    ,
    N. A. Fleck
    DOI: 10.1115/1.2198549
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The finite element method is used to evaluate the underwater blast resistance of monolithic beams and sandwich beams containing prismatic lattice cores (Y-frame and corrugated core) and an ideal foam core. Calculations are performed on both free-standing and end-clamped beams, and fluid-structure interaction effects are accounted for. It is found that the degree of core compression in the free-standing sandwich beam is sensitive to core strength, yet the transmitted impulse is only mildly sensitive to the type of sandwich core. Clamped sandwich beams significantly outperform clamped monolithic beams of equal mass, particularly for stubby beams. The Fleck and Deshpande analytical model for the blast response of sandwich beams is critically assessed by determining the significance of cross-coupling between the three stages of response: in stage I the front face is accelerated by the fluid up to the point of first cavitation, stage II involves compression of the core until the front and back faces have an equal velocity, and in stage III the sandwich beam arrests by a combination of beam bending and stretching. The sensitivity of the response to the relative magnitude of these time scales is assessed by appropriately chosen numerical simulations. Coupling between stages I and II increases the level of transmitted impulse by the fluid by 20–30% for a wide range of core strengths, for both the free-standing and clamped beams. Consequently, the back face deflection of the clamped sandwich beam exceeds that of the fully decoupled model. For stubby beams with a Y-frame and corrugated core, strong coupling exists between the core compression phase (stage II) and the beam bending/stretching phase (stage III); this coupling is beneficial as it results in a reduced deflection of the back (distal) face. In contrast, the phases of core compression (stage II) and beam bending/stretching (stage III) are decoupled for slender beams. The significance of the relative time scales for the three stages of response of the clamped beams are summarized on a performance map that takes as axes the ratios of the time scales.
    keyword(s): Momentum , Fluids , Electrical resistance , Structural frames , Impulse (Physics) , Engineering simulation , Compression , Deflection , Fluid structure interaction , Waves , Materials properties AND Cavitation ,
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      The Underwater Blast Resistance of Metallic Sandwich Beams With Prismatic Lattice Cores

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    http://yetl.yabesh.ir/yetl1/handle/yetl/135158
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    • Journal of Applied Mechanics

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    contributor authorG. J. McShane
    contributor authorV. S. Deshpande
    contributor authorN. A. Fleck
    date accessioned2017-05-09T00:22:36Z
    date available2017-05-09T00:22:36Z
    date copyrightMarch, 2007
    date issued2007
    identifier issn0021-8936
    identifier otherJAMCAV-26621#352_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/135158
    description abstractThe finite element method is used to evaluate the underwater blast resistance of monolithic beams and sandwich beams containing prismatic lattice cores (Y-frame and corrugated core) and an ideal foam core. Calculations are performed on both free-standing and end-clamped beams, and fluid-structure interaction effects are accounted for. It is found that the degree of core compression in the free-standing sandwich beam is sensitive to core strength, yet the transmitted impulse is only mildly sensitive to the type of sandwich core. Clamped sandwich beams significantly outperform clamped monolithic beams of equal mass, particularly for stubby beams. The Fleck and Deshpande analytical model for the blast response of sandwich beams is critically assessed by determining the significance of cross-coupling between the three stages of response: in stage I the front face is accelerated by the fluid up to the point of first cavitation, stage II involves compression of the core until the front and back faces have an equal velocity, and in stage III the sandwich beam arrests by a combination of beam bending and stretching. The sensitivity of the response to the relative magnitude of these time scales is assessed by appropriately chosen numerical simulations. Coupling between stages I and II increases the level of transmitted impulse by the fluid by 20–30% for a wide range of core strengths, for both the free-standing and clamped beams. Consequently, the back face deflection of the clamped sandwich beam exceeds that of the fully decoupled model. For stubby beams with a Y-frame and corrugated core, strong coupling exists between the core compression phase (stage II) and the beam bending/stretching phase (stage III); this coupling is beneficial as it results in a reduced deflection of the back (distal) face. In contrast, the phases of core compression (stage II) and beam bending/stretching (stage III) are decoupled for slender beams. The significance of the relative time scales for the three stages of response of the clamped beams are summarized on a performance map that takes as axes the ratios of the time scales.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleThe Underwater Blast Resistance of Metallic Sandwich Beams With Prismatic Lattice Cores
    typeJournal Paper
    journal volume74
    journal issue2
    journal titleJournal of Applied Mechanics
    identifier doi10.1115/1.2198549
    journal fristpage352
    journal lastpage364
    identifier eissn1528-9036
    keywordsMomentum
    keywordsFluids
    keywordsElectrical resistance
    keywordsStructural frames
    keywordsImpulse (Physics)
    keywordsEngineering simulation
    keywordsCompression
    keywordsDeflection
    keywordsFluid structure interaction
    keywordsWaves
    keywordsMaterials properties AND Cavitation
    treeJournal of Applied Mechanics:;2007:;volume( 074 ):;issue: 002
    contenttypeFulltext
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