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Aluminium Design and Construction John Dwight

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Figure 9.4 Fundamental buckling modes for a compression member.<br />

the torsional mode never governs when the section is thick, as in heavy<br />

gauge (hot-rolled) steel. It becomes more likely as the thickness decreases,<br />

<strong>and</strong> for thin-walled members it is often critical, as also in light gauge<br />

(cold-formed) steel. The checking of torsional buckling tends to be<br />

laborious. Here we follow the treatment given in BS.8118, which is<br />

more comprehensive than any provided in previous codes. The calculations<br />

involve the use of torsional section properties, which may not be familiar<br />

to some designers. Chapter 10 provides help for evaluating these.<br />

9.6.2 Interaction with flexure<br />

A tiresome complication with torsional buckling is that the fundamental<br />

buckling modes often interact, depending on the degree of symmetry<br />

in the section (Figure 9.5):<br />

1. Bisymmetric section. The three modes are independent (no interaction);<br />

2. Radial-symmetric section. As for 1;<br />

3. Skew-symmetric section. As for 1;<br />

4. Monosymmetric section. Interaction occurs between pure torsional<br />

buckling about the shear centre S <strong>and</strong> column buckling about the<br />

axis of symmetry ss;<br />

5. Asymmetric section. All three modes interact.<br />

The effect of interaction is to make the section rotate about a point other<br />

than the shear centre S, as illustrated for a monosymmetric section in<br />

Figure 9.5 Degrees of symmetry for strut sections: (1) bisymmetric; (2) radial-symmetric;<br />

(3) skew-symmetric; (4) monosymmetric; (5) asymmetric.<br />

Copyright 1999 by Taylor & Francis Group. All Rights Reserved.

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