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    Fatigue Crack Growth Properties of a Cryogenic Structural Steel at Liquid Helium Temperature

    Source: Journal of Engineering Materials and Technology:;1996:;volume( 118 ):;issue: 001::page 109
    Author:
    Shinji Konosu
    ,
    Yoshihiko Nunoya
    ,
    Hideo Nakajima
    ,
    Tomohiro Kishiro
    ,
    Ogi Ivano
    ,
    Hiroshi Tsuji
    DOI: 10.1115/1.2805922
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The structural materials of the coils of superconducting magnets utilized in thermonuclear fusion reactors are used at liquid helium (4.2 K) temperatures and are subjected to repeated thermal stresses and electromagnetic forces. A high strength, high toughness austenitic stainless steel (12Cr-12Ni-10Mn-5Mo-0.2N) has recently been developed for large, thick-walled components used in such environments. This material is non-magnetic even when subjected to processing and, because it is a forging material, it is advantageous as a structural material for large components. In the current research, a large forging of 12Cr-12Ni-10Mn-5Mo-0.2N austenitic stainless steel, was fabricated to a thickness of 250 mm, which is typical of section thicknesses encountered in actual equipment. The tensile fatigue crack growth properties of the forging were examined at liquid helium temperature as function of specimen location across the thickness of the forging. There was virtually no evidence of variation in tensile strength or fatigue crack growth properties attributable to different sampling locations in the thickness direction and no effect of thickness due to the forging or solution treatment associated with large forgings was observed. It has been clarified that there are cases in which small scale yielding (SSY) conditions are not fulfilled when stress ratios are large. ΔJ was introduced in order to achieve unified expression inclusive of these regions and, by expressing crack growth rate accordingly, the following formula was obtained at the second stage (middle range). da/dN = CJ ΔJm J , CJ = AJ /(ΔJ0 )m J , where, AJ = 1.47 × 10−5 mm/cycle, ΔJ0 = 2.42 × 103 N/m.
    keyword(s): Temperature , Structural steel , Fatigue cracks , Helium , Forging , Thickness , Stainless steel , Tensile strength , Formulas , Toughness , Superconducting magnets , Stress , Fusion reactors , Forgings (Products) , Thermal stresses , Sampling (Acoustical engineering) , Electromagnetic force , Fracture (Materials) AND Cycles ,
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      Fatigue Crack Growth Properties of a Cryogenic Structural Steel at Liquid Helium Temperature

    URI
    https://yetl.yabesh.ir/yetl1/handle/yetl/117085
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    • Journal of Engineering Materials and Technology

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    contributor authorShinji Konosu
    contributor authorYoshihiko Nunoya
    contributor authorHideo Nakajima
    contributor authorTomohiro Kishiro
    contributor authorOgi Ivano
    contributor authorHiroshi Tsuji
    date accessioned2017-05-08T23:50:24Z
    date available2017-05-08T23:50:24Z
    date copyrightJanuary, 1996
    date issued1996
    identifier issn0094-4289
    identifier otherJEMTA8-26976#109_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/117085
    description abstractThe structural materials of the coils of superconducting magnets utilized in thermonuclear fusion reactors are used at liquid helium (4.2 K) temperatures and are subjected to repeated thermal stresses and electromagnetic forces. A high strength, high toughness austenitic stainless steel (12Cr-12Ni-10Mn-5Mo-0.2N) has recently been developed for large, thick-walled components used in such environments. This material is non-magnetic even when subjected to processing and, because it is a forging material, it is advantageous as a structural material for large components. In the current research, a large forging of 12Cr-12Ni-10Mn-5Mo-0.2N austenitic stainless steel, was fabricated to a thickness of 250 mm, which is typical of section thicknesses encountered in actual equipment. The tensile fatigue crack growth properties of the forging were examined at liquid helium temperature as function of specimen location across the thickness of the forging. There was virtually no evidence of variation in tensile strength or fatigue crack growth properties attributable to different sampling locations in the thickness direction and no effect of thickness due to the forging or solution treatment associated with large forgings was observed. It has been clarified that there are cases in which small scale yielding (SSY) conditions are not fulfilled when stress ratios are large. ΔJ was introduced in order to achieve unified expression inclusive of these regions and, by expressing crack growth rate accordingly, the following formula was obtained at the second stage (middle range). da/dN = CJ ΔJm J , CJ = AJ /(ΔJ0 )m J , where, AJ = 1.47 × 10−5 mm/cycle, ΔJ0 = 2.42 × 103 N/m.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleFatigue Crack Growth Properties of a Cryogenic Structural Steel at Liquid Helium Temperature
    typeJournal Paper
    journal volume118
    journal issue1
    journal titleJournal of Engineering Materials and Technology
    identifier doi10.1115/1.2805922
    journal fristpage109
    journal lastpage113
    identifier eissn1528-8889
    keywordsTemperature
    keywordsStructural steel
    keywordsFatigue cracks
    keywordsHelium
    keywordsForging
    keywordsThickness
    keywordsStainless steel
    keywordsTensile strength
    keywordsFormulas
    keywordsToughness
    keywordsSuperconducting magnets
    keywordsStress
    keywordsFusion reactors
    keywordsForgings (Products)
    keywordsThermal stresses
    keywordsSampling (Acoustical engineering)
    keywordsElectromagnetic force
    keywordsFracture (Materials) AND Cycles
    treeJournal of Engineering Materials and Technology:;1996:;volume( 118 ):;issue: 001
    contenttypeFulltext
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