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The Design of Modern Steel Bridges - TEDI

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124 <strong>The</strong> <strong>Design</strong> <strong>of</strong> <strong>Modern</strong> <strong>Steel</strong> <strong>Bridges</strong><br />

Figure 5.17 Behaviour <strong>of</strong> plates in compression, with and without welding<br />

residual stress. Plate with (a) stable post-buckling behaviour, (b) unstable postbuckling<br />

behaviour.<br />

Welding residual stresses are less important for plates subjected to in-plane<br />

shear or bending stress than plates under longitudinal compression. This is<br />

because the applied stresses and the welding residual stresses are likely to be <strong>of</strong><br />

different natures in different parts <strong>of</strong> the plates.<br />

5.4.4 Effects <strong>of</strong> initial out-<strong>of</strong>-plane imperfections<br />

Sections 5.4.1 and 5.4.2 dealt with the buckling behaviour <strong>of</strong> ideally flat plate<br />

panels, i.e. plates without any initial out-<strong>of</strong>-plane deviations. Plates in real-life<br />

fabricated structures are likely to have some initial out-<strong>of</strong>-plane deviations.<br />

Instead <strong>of</strong> the ideal bilinear behaviour shown in Fig. 5.12(b), the real behaviour<br />

<strong>of</strong> such plates will be as shown in graph (b) <strong>of</strong> Fig. 5.18. <strong>The</strong> initial out-<strong>of</strong>plane<br />

deviation will start growing in depth from the beginning <strong>of</strong> loading.<br />

<strong>The</strong>re will not occur any sudden change in the rate <strong>of</strong> in-plane or out-<strong>of</strong>-plane<br />

deformation at the theoretical elastic critical buckling stress, but the rate will<br />

gradually increase until the maximum resistance or ultimate strength <strong>of</strong> the<br />

plate is reached. <strong>The</strong>reafter as the resistance falls, the in-plane and out-<strong>of</strong>-plane<br />

deformations continue to grow.<br />

<strong>The</strong> in-plane edge conditions <strong>of</strong> the plate influence its behaviour right from<br />

the beginning. As in the case <strong>of</strong> perfectly flat plates, the ultimate strength is<br />

reached by a combination <strong>of</strong> redistribution <strong>of</strong> the in-plane applied stresses<br />

and the growth <strong>of</strong> bending stresses due to the out-<strong>of</strong>-plane deviations. <strong>The</strong>

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