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Aluminium Design and Construction John Dwight

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Note that when P is tensile, the first term in equation (9.21) should<br />

be put equal to zero. Also, if the section is of a type not prone to LT<br />

buckling, p b is put equal to M C /S where M c is as in check B.<br />

9.7.5 Alternative treatment (P+uniaxial M)<br />

The checks A <strong>and</strong> B tend to be oversafe when applied to fully-compact<br />

profiles, <strong>and</strong> for these a more realistic result can be obtained by using<br />

a direct plastic calculation instead:<br />

(9.22a)<br />

(9.22b)<br />

where p o is the limiting material stress for bending (Section 5.3), <strong>and</strong> S p<br />

is a suitably reduced value for the plastic modulus that allows for the<br />

presence of P (Section 10.2.3). S p is different for the two checks.<br />

Figure 9.17 compares results thus obtained with those given by the<br />

British St<strong>and</strong>ard rule. It covers check A for a fully-compact box section,<br />

<strong>and</strong> shows how the reduced moment resistance of the section (in the<br />

presence of axial load) varies with P. It is seen that the British St<strong>and</strong>ard<br />

rule can underestimate by as much as 20%.<br />

9.7.6 Interaction formulae (P+biaxial M)<br />

We now consider the case when the applied moment acts about an axis<br />

mm inclined � at to the major principal axis xx (Figure 9.18). Section<br />

classification follows the same principles as those given in Section 9.7.3,<br />

a single classification being needed which corresponds to the particular<br />

Figure 9.17 Reduced moment resistance of a fully-compact square box cross-section in<br />

the presence of axial load: (1) BS 8118 rule (equation 9.18); (2) Direct plastic calculation<br />

(equation (9.22a)).<br />

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

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