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    Plastic Yielding as a Phase Transition

    Source: Journal of Applied Mechanics:;1999:;volume( 066 ):;issue: 002::page 289
    Author:
    M. Ortiz
    DOI: 10.1115/1.2791048
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: A statistical mechanical theory of forest hardening is developed in which yielding arises as a phase transition. For simplicity, we consider the case of a single dislocation loop moving on a slip plane through randomly distributed forest dislocations, which we treat as point obstacles. The occurrence of slip at the sites occupied by these obstacles is assumed to require the expenditure of a certain amount of work commensurate with the strength of the obstacle. The case of obstacles of infinite strength is treated in detail. We show that the behavior of the dislocation loop as it sweeps the slip plane under the action of a resolved shear stress is identical to that of a lattice gas, or, equivalently, to that of the two-dimensional spin-1/2 Ising model. In particular, there exists a critical temperature Tc below which the system exhibits a yield point, i.e., the slip strain increases sharply when the applied resolved shear stress attains a critical value. Above the critical temperature the yield point disappears and the slip strain depends continuously on the applied stress. The critical exponents, which describe the behavior of the system near the critical temperature, coincide with those of the two-dimensional spin-1/2 Ising model.
    keyword(s): Phase transitions , Stress , Dislocations , Temperature , Yield point , Ising model , Shear (Mechanics) , Particle spin AND Hardening ,
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      Plastic Yielding as a Phase Transition

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    contributor authorM. Ortiz
    date accessioned2017-05-08T23:58:49Z
    date available2017-05-08T23:58:49Z
    date copyrightJune, 1999
    date issued1999
    identifier issn0021-8936
    identifier otherJAMCAV-26470#289_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/121666
    description abstractA statistical mechanical theory of forest hardening is developed in which yielding arises as a phase transition. For simplicity, we consider the case of a single dislocation loop moving on a slip plane through randomly distributed forest dislocations, which we treat as point obstacles. The occurrence of slip at the sites occupied by these obstacles is assumed to require the expenditure of a certain amount of work commensurate with the strength of the obstacle. The case of obstacles of infinite strength is treated in detail. We show that the behavior of the dislocation loop as it sweeps the slip plane under the action of a resolved shear stress is identical to that of a lattice gas, or, equivalently, to that of the two-dimensional spin-1/2 Ising model. In particular, there exists a critical temperature Tc below which the system exhibits a yield point, i.e., the slip strain increases sharply when the applied resolved shear stress attains a critical value. Above the critical temperature the yield point disappears and the slip strain depends continuously on the applied stress. The critical exponents, which describe the behavior of the system near the critical temperature, coincide with those of the two-dimensional spin-1/2 Ising model.
    publisherThe American Society of Mechanical Engineers (ASME)
    titlePlastic Yielding as a Phase Transition
    typeJournal Paper
    journal volume66
    journal issue2
    journal titleJournal of Applied Mechanics
    identifier doi10.1115/1.2791048
    journal fristpage289
    journal lastpage298
    identifier eissn1528-9036
    keywordsPhase transitions
    keywordsStress
    keywordsDislocations
    keywordsTemperature
    keywordsYield point
    keywordsIsing model
    keywordsShear (Mechanics)
    keywordsParticle spin AND Hardening
    treeJournal of Applied Mechanics:;1999:;volume( 066 ):;issue: 002
    contenttypeFulltext
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