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Aluminium Design and Construction John Dwight

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We now turn to monosymmetric sections (Figure 10.2(c)). The above<br />

treatment holds valid for these in principle, but the calculation is longer,<br />

because we need two parameters (w, z) to specify the neutral axis nn. The<br />

whole section is split up into convenient elements, none of which must<br />

straddle nn. A convenient pair of axes OX <strong>and</strong> OY is selected, enabling<br />

expressions for S x <strong>and</strong> S y (in terms of w <strong>and</strong> z) to be obtained as follows:<br />

(10.6)<br />

where: AE =area of an element taken positive for compression material<br />

<strong>and</strong> negative for tensile, <strong>and</strong> XE , YE =coordinates of an elements’s centroid<br />

E referred to the axes OX <strong>and</strong> OY, with signs taken accordingly. The<br />

summations are performed for the whole section. The dimensions w<br />

<strong>and</strong> z (defining the position of nn) are then obtained by solving a pair<br />

of simultaneous equations based on the following requirements:<br />

1. The areas either side of nn must be equal.<br />

2. Equation (10.4) must be satisfied.<br />

Having thus found w <strong>and</strong> z, the required modulus Sm is determined from<br />

expression (10.5) as before. The right answer will be obtained, however<br />

the axes OX <strong>and</strong> OY are chosen, provided all signs are taken correctly.<br />

Unsymmetrical sections can be dealt with using the same kind of<br />

approach.<br />

10.2.3 Bending with axial force<br />

The reduced moment capacity of a fully compact section in the presence<br />

of a coincident axial force P can be obtained by using a modified value<br />

for the plastic section modulus, as required in Section 9.7.5 (expressions<br />

(9.22)) <strong>and</strong> also in Section 9.7.7(1).<br />

Consider first the symmetrical bending case when the moment M<br />

acts about an axis of symmetry ss (Figure 10.3(a)). The aim is to find<br />

the modified plastic modulus S p which allows for the presence of P.<br />

The figure shows the (idealized) plastic pattern of stress at failure<br />

with assumed rectangular stress-blocks, in which we identify regions<br />

1, 2, 3. Region 2 extends equally either side of ss, the regions 1 <strong>and</strong><br />

3 being therefore of equal area. Region 2 may be regarded as carrying<br />

P, while 1 <strong>and</strong> 3 look after M. Referring to Section 9.7.5 the stress on<br />

region 1 is assumed to be p a for check A (localized failure), or p o for<br />

check B (general yielding). The height of the neutral axis nn is selected<br />

so that the force produced by the stress on region 1 (=its area×p a or<br />

p o ) is equal to � m P. The required value of S p is then simply taken as the<br />

plastic modulus contributed by regions 1 <strong>and</strong> 3. Note that the value<br />

thus obtained is slightly different for the two checks. (P is axial force<br />

under factored loading.)<br />

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

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