2013
DOI: 10.1016/j.tws.2013.08.014
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Behavior of thin-walled circular hollow section tubes subjected to bending

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Cited by 105 publications
(42 citation statements)
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“…It was also found that the ultimate strength of a shell with a cutout on the compression side was less than for a cutout on the tension side, and the ultimate strength increased when a cutout was close to the end of the clamped shell. Guo et al (2013) found that an increase in the D/t ratio resulted in a more pronounced local buckling phenomenon, with the stiffeners increasing the loadcarrying capacity while improving the ductility.…”
Section: Literature Reviewmentioning
confidence: 99%
See 1 more Smart Citation
“…It was also found that the ultimate strength of a shell with a cutout on the compression side was less than for a cutout on the tension side, and the ultimate strength increased when a cutout was close to the end of the clamped shell. Guo et al (2013) found that an increase in the D/t ratio resulted in a more pronounced local buckling phenomenon, with the stiffeners increasing the loadcarrying capacity while improving the ductility.…”
Section: Literature Reviewmentioning
confidence: 99%
“…For a couple of decades, a number of studies were conducted to provide buckling analyses of circular cylindrical shells (Brazier 1927;Reissner 1961;Seide & Weingarten 1961;Fabian 1977;Gellin 1980) with cutouts under axial compression (Schenk & Schuёller 2007;Shariati &Rokhi 2010;Ghazijahani et al 2015) and pure bending (Yeh et al 1999;Dimopoulos & Gantes 2012, 2015Guo et al 2013;.…”
Section: Introductionmentioning
confidence: 99%
“…Local buckling appears when the bending ultimate moment reaches a critical value, and thereafter the bending moment declines and bending instability occurs. For a rigid-perfectly plastic pipe with the original radius R, wall thickness t and length l, when it is subjected to bending load and enters into the fully plastic state, the pure bending moment due to cross-sectional ovalization can be written as [23,24] in which a i and b i are the lengths of the internal longer semi-axis and shorter semi-axis. a and b are the lengths of the external longer semi-axis and shorter semi-axis, a = (a i + t), b = b i + t), respectively.…”
Section: New Expression For Apparent Strain Of a Pipe At Plastic-bendmentioning
confidence: 99%
“…Local buckling appears when the bending ultimate moment reaches to a critical value, and thereafter bending moment declines and the bending instability occurs. For a rigid -perfectly plastic pipe with the original radius R, wall thickness , and length , when it is subjected bending load and enters into fully plastic state, the pure bending moment due to cross section ovalization could be written as [13,14] …”
Section: Strain Energy Rate Corresponding To Pure Bendingmentioning
confidence: 99%