1998
DOI: 10.1016/s0045-7949(97)00112-0
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Perturbation Approach to Elastic Post-Buckling Analysis

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Cited by 58 publications
(34 citation statements)
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“…(ii) Perform the buckling search (6b); this corresponds to a nonlinear eigenvalue problem which can be, however, easily solved, as described in [Casciaro et al 1998], by an iterative scheme only requiring matrix K −1 0 be available in factorized form, as it already is from the previous step. (iii) Solve orthogonal equations (6f); they correspond to a linear system where the right-hand vectors p i j are obtained as a function of v i by an element-by-element assembling process similar to that used for obtaining s [u]; as K b ≈ K 0 within the orthogonal space ᐃ, its solution can be conveniently obtained, as described in [Casciaro et al 1998], through a modified Newton-like iteration scheme exploiting K 0 as an iteration matrix (see [Casciaro 2004] for further insights).…”
mentioning
confidence: 99%
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“…(ii) Perform the buckling search (6b); this corresponds to a nonlinear eigenvalue problem which can be, however, easily solved, as described in [Casciaro et al 1998], by an iterative scheme only requiring matrix K −1 0 be available in factorized form, as it already is from the previous step. (iii) Solve orthogonal equations (6f); they correspond to a linear system where the right-hand vectors p i j are obtained as a function of v i by an element-by-element assembling process similar to that used for obtaining s [u]; as K b ≈ K 0 within the orthogonal space ᐃ, its solution can be conveniently obtained, as described in [Casciaro et al 1998], through a modified Newton-like iteration scheme exploiting K 0 as an iteration matrix (see [Casciaro 2004] for further insights).…”
mentioning
confidence: 99%
“…(iii) Solve orthogonal equations (6f); they correspond to a linear system where the right-hand vectors p i j are obtained as a function of v i by an element-by-element assembling process similar to that used for obtaining s [u]; as K b ≈ K 0 within the orthogonal space ᐃ, its solution can be conveniently obtained, as described in [Casciaro et al 1998], through a modified Newton-like iteration scheme exploiting K 0 as an iteration matrix (see [Casciaro 2004] for further insights).…”
mentioning
confidence: 99%
“…The details descriptions of this method can be found in the monographs: van der Heijden (2009), Thompson and Hunt (1973) or Kubiak (2013). Applicability of an asymptotic expansion for elastic buckling problems with mode interaction was discussed in many papers, for instance: Tvergaard (1973aTvergaard ( , 1973b, Koiter and Pignataro (1974), Byskov (1979Byskov ( , 1988, Sridharan (1983), Sridharan (1985a, 1985b), Pignataro and Luongo (1985, 1987a, 1987b, Casciaro et al (1998), Mollman (1989a, 1989b), Garcea et al (1999Garcea et al ( , 2009), Barbero et al (2014).…”
Section: Coupled Buckling Of Thin-walled Structuresmentioning
confidence: 99%
“…As a result, the prebuckling, buckling and initial postbuckling behaviors are captured in just three solution steps compared to multiple iterations required in incremental algorithms. Koiter's approach was applied by Stein 33 for rectangular isotropic plates, Chandra & Raju 34 for symmetrically laminated orthotropic plates, and was extended in an optimization framework by Wu et al 35 Furthermore, Koiter's perturbation technique lends itself to robust implementation in numerical solution techniques such as the Finite Element Method (FEM) 36 and the Differential Quadrature Method (DQM). 37 Recently, Koiter's perturbation scheme was coupled with a Newton-Raphson iterative solver in order to combine the merits of both asymptotic and path-following techniques, thereby allowing efficient modeling of nonlinear prebuckling paths and limit-point buckling.…”
Section: Iib Koiter's Perturbation Approachmentioning
confidence: 99%