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Aluminium Design and Construction John Dwight

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For sections where the position of the shear-centre S is known, equation<br />

(10.29) enables H to be found directly. For other sections, it is first<br />

necessary to locate S.<br />

10.5.5 Bisymmetric <strong>and</strong> radial-symmetric sections<br />

For these, S lies at the point of symmetry, which is also the point of<br />

zero warping. We take O at the same position, giving wo =0.<br />

For the bisymmetric case (Figure 10.17(a)), the elements are numbered<br />

in one quadrant only. The necessary summation in equation (10.29) is<br />

then made just for these elements, <strong>and</strong> the result multiplied by 4 to<br />

obtain H. Note that element 1 makes no contribution because it does<br />

not warp.<br />

Figure 10.17(b) shows the radial-symmetric case, consisting of n equally<br />

spaced identical arms, each symmetrical about a radius. For this, the<br />

summation in equation (10.29) can be made for the elements lying one<br />

side of one arm, <strong>and</strong> the result then multiplied by 2n.<br />

Figure 10.17 Symmetric sections: (a) bisymmetric; (b) radial-symmetric; (c) skew-symmetric;<br />

(d) skew-radial-symmetric.<br />

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

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