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    Pipe Deformation During a Running Shear Fracture in Line Pipe

    Source: Journal of Engineering Materials and Technology:;1974:;volume( 096 ):;issue: 004::page 309
    Author:
    K. D. Ives
    ,
    A. K. Shoemaker
    ,
    R. F. McCartney
    DOI: 10.1115/1.3443246
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Under sponsorship of the American Iron and Steel Institute, U. S. Steel Research has been conducting full-scale burst tests of large-diameter submerged-arc-welded line pipe to determine the toughness required to arrest running shear fractures for different design conditions. As part of that program, the pipe were instrumented with crack detectors, strain gages, and pressure transducers to determine the crack velocities and the actual pipe deformation and strain fields associated with the shear fracture propagating along the top of the pipe. This paper summarizes the test data that document the manner in which the pipe deforms during this type of crack propagation. The data show that for a propagating shear fracture, each of four different locations along the pipe length (relative to the crack tip) has a distinctive type of pipe deformation. For a location many pipe diameters ahead of the crack tip, the circumferential strain first decreases because of flexural waves associated with the initiation process and then continues to decrease in proportion to the local gas decompression; however, the longitudinal strain continuously increases because of a longitudinal “tongue” of tensile straining on the top of the pipe caused by pressure-induced opening of the flaps of the pipe on both sides of the fracture behind the crack tip. At a distance about two diameters ahead of the crack tip, the pipe cross section becomes oval, and in the presence of this deformation the strain field is no longer determined by the local pressure; in fact, the circumferential strain is near zero at a distance two diameters ahead of the crack. The oval pipe shape ahead of the crack tip is caused by the venting of the gas behind the crack tip which creates a downward reactive force on the bottom portion of the pipe. Opening at the crack tip is the result of tensile straining caused by circumferential and radial displacement of the flaps behind the crack tip. Thus it is believed that the action of the pipe-wall flaps behind the crack tip provides the primary force driving the crack down the top of the pipe.
    keyword(s): Deformation , Shear (Mechanics) , Fracture (Process) , Pipes , Force , Pressure , Steel , Sensors , Pressure transducers , Waves , Design , Crack propagation , Displacement , Iron , Shapes , Strain gages AND Toughness ,
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      Pipe Deformation During a Running Shear Fracture in Line Pipe

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    http://yetl.yabesh.ir/yetl1/handle/yetl/164795
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    • Journal of Engineering Materials and Technology

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    contributor authorK. D. Ives
    contributor authorA. K. Shoemaker
    contributor authorR. F. McCartney
    date accessioned2017-05-09T01:38:11Z
    date available2017-05-09T01:38:11Z
    date copyrightOctober, 1974
    date issued1974
    identifier issn0094-4289
    identifier otherJEMTA8-26838#309_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/164795
    description abstractUnder sponsorship of the American Iron and Steel Institute, U. S. Steel Research has been conducting full-scale burst tests of large-diameter submerged-arc-welded line pipe to determine the toughness required to arrest running shear fractures for different design conditions. As part of that program, the pipe were instrumented with crack detectors, strain gages, and pressure transducers to determine the crack velocities and the actual pipe deformation and strain fields associated with the shear fracture propagating along the top of the pipe. This paper summarizes the test data that document the manner in which the pipe deforms during this type of crack propagation. The data show that for a propagating shear fracture, each of four different locations along the pipe length (relative to the crack tip) has a distinctive type of pipe deformation. For a location many pipe diameters ahead of the crack tip, the circumferential strain first decreases because of flexural waves associated with the initiation process and then continues to decrease in proportion to the local gas decompression; however, the longitudinal strain continuously increases because of a longitudinal “tongue” of tensile straining on the top of the pipe caused by pressure-induced opening of the flaps of the pipe on both sides of the fracture behind the crack tip. At a distance about two diameters ahead of the crack tip, the pipe cross section becomes oval, and in the presence of this deformation the strain field is no longer determined by the local pressure; in fact, the circumferential strain is near zero at a distance two diameters ahead of the crack. The oval pipe shape ahead of the crack tip is caused by the venting of the gas behind the crack tip which creates a downward reactive force on the bottom portion of the pipe. Opening at the crack tip is the result of tensile straining caused by circumferential and radial displacement of the flaps behind the crack tip. Thus it is believed that the action of the pipe-wall flaps behind the crack tip provides the primary force driving the crack down the top of the pipe.
    publisherThe American Society of Mechanical Engineers (ASME)
    titlePipe Deformation During a Running Shear Fracture in Line Pipe
    typeJournal Paper
    journal volume96
    journal issue4
    journal titleJournal of Engineering Materials and Technology
    identifier doi10.1115/1.3443246
    journal fristpage309
    journal lastpage317
    identifier eissn1528-8889
    keywordsDeformation
    keywordsShear (Mechanics)
    keywordsFracture (Process)
    keywordsPipes
    keywordsForce
    keywordsPressure
    keywordsSteel
    keywordsSensors
    keywordsPressure transducers
    keywordsWaves
    keywordsDesign
    keywordsCrack propagation
    keywordsDisplacement
    keywordsIron
    keywordsShapes
    keywordsStrain gages AND Toughness
    treeJournal of Engineering Materials and Technology:;1974:;volume( 096 ):;issue: 004
    contenttypeFulltext
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