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Steel Designers Manual - TheBestFriend.org

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This material is copyright - all rights reserved. Reproduced under licence from The <strong>Steel</strong> Construction Institute on 12/2/2007<br />

To buy a hardcopy version of this document call 01344 872775 or go to http://shop.steelbiz.<strong>org</strong>/<br />

<strong>Steel</strong> <strong>Designers</strong>' <strong>Manual</strong> - 6th Edition (2003)<br />

514 Members with compression and moments<br />

Fl<br />

PC<br />

M1<br />

corresponding<br />

value of M Mc<br />

(a) (b)<br />

Fig. 18.3 Concept of interaction diagrams for combined loading: (a) two-dimensional, (b)<br />

three-dimensional<br />

is possible, the member slenderness and the cross-sectional shape. Design methods<br />

for beam-columns must therefore seek to balance the conflicting requirements of<br />

rigour, which would try to adjust the form of the design boundary of Fig. 18.3 to<br />

reflect the influence of each of these factors, and simplicity. However, some appreciation<br />

of the role of each factor is necessary if even the simplest design approach<br />

is to be properly appreciated and applied.<br />

The importance of member slenderness may be appreciated readily with reference<br />

to the two-dimensional example illustrated in Fig. 18.4. The member is loaded<br />

by compression plus equal and opposite end moments and is assumed to respond<br />

simply by deflecting in the plane of the applied loading. Under the action of the<br />

applied moments bending occurs, leading to a lateral deflection v. The moment at<br />

any point within the length comprises two components: a constant primary moment<br />

M due to the applied end moments plus a secondary moment Fv due to the axial<br />

load F acting through the lateral deflection v. Summing the effects of compression<br />

and bending gives<br />

FP / + M / M =10 .<br />

(18.1)<br />

c max c<br />

in which Pc and Mc are the resistance as a strut and a beam respectively and Mmax<br />

is the total moment.<br />

Analysis of beam-column problems shows that Mmax may be closely approximated<br />

by<br />

Mmax = M/ ( 1 -F/<br />

Pcr)<br />

(18.2)

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