1984
DOI: 10.1243/03093247v194221
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A linear programming upper bound approach to the shakedown limit of thin shells subjected to variable thermal loading

Abstract: This paper describes an upper bound technique for the evaluation of the shakedown limit of thin cyclindrical shells subject to thermal loading. The method is based upon the upper bound kinematic shakedown theorem of Koiter. By suitable choice of displacement field, in a finite element form, and yield surface, the problem is reduced to a linear programming problem. A number of solutions are presented involving a tube subjected to a moving temperature front which indicates that the technique provides, in an efic… Show more

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Cited by 35 publications
(12 citation statements)
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“…In previous kinematic shakedown analyses, linear programming techniques were developed by using piece-wise linear (Tresca) or linearized yield criterion, e.g. [11,23]. The application of von Mises criterion leads to a nonlinear mathematical programming problem, the solution of which in practical engineering applications with complex structures and loading still represents a challenge.…”
mentioning
confidence: 99%
“…In previous kinematic shakedown analyses, linear programming techniques were developed by using piece-wise linear (Tresca) or linearized yield criterion, e.g. [11,23]. The application of von Mises criterion leads to a nonlinear mathematical programming problem, the solution of which in practical engineering applications with complex structures and loading still represents a challenge.…”
mentioning
confidence: 99%
“…In what follows, the yield function values are sometimes denoted as : 1 5 4 38 9 8. The yield function is assumed to be strictly convex in the argument 4 3, and the inequality …”
Section: 65374mentioning
confidence: 99%
“…Only very few experimental results with cyclic thermal loading have been reported in Ponter (1983), Leers (1985) and Lang et al (2001). Numerical methods therefore have received much attention: Penny (1967, 1969), Sagar and Payne (1975), Goodman (1978), Karadeniz and Ponter (1984), Ponter and Karadeniz (1985a,b). If the yield stress is a linear or a concave function of temperature, linear or convex 0020-7683/$ -see front matter Ó 2006 Elsevier Ltd. All rights reserved.…”
Section: Introductionmentioning
confidence: 99%