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Aluminium Design and Construction John Dwight

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Figure 8.11 Shear buckling stress for stiffened webs (without tension-field action).<br />

When transverse stiffeners are fitted, an improved value of p v1 may<br />

be read from Figure 8.11, in which a is the stiffener spacing. Alternatively<br />

the designer may use the equations on which the figure is based:<br />

(8.14a)<br />

(8.14b)<br />

For a web fitted with tongue plate or plates (Figure 8.10(b)), it is necessary<br />

to sum the web <strong>and</strong> tongue contributions. This may be done as follows,<br />

provided the tongue plates are properly designed (Section 8.6.2):<br />

V c =V cw +V ct<br />

(8.15)<br />

where: V cw =value given by (8.12) taking d as the depth between tongues,<br />

V ct =Σ A t p vt<br />

� A t =total effective area of tongue plates,<br />

p vt =limiting stress in shear for tongue material.<br />

In a multi-web beam, V c may be taken as the sum of the values found<br />

for the individual webs, using expression (8.12) or (8.15) as appropriate.<br />

8.3.6 Web buckling, tension-field action<br />

Very slender stiffened webs can often accept a great increase in shear<br />

force above the initial buckling load before they finally fail. This results<br />

from the development of a diagonal tension field as the buckles develop<br />

(Figure 8.12). The designer can take advantage of this by using the treatment<br />

below, based on the ‘Cardiff model’ of Rockey <strong>and</strong> Evans [15], which<br />

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

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