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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 />

Fig. 9.27 Unit load method<br />

jPi r2 jFs<br />

B C D<br />

iagram<br />

IA<br />

11<br />

B<br />

qram<br />

Analysis of skeletal structures 315<br />

The total strain energy of an elastic system is given by the sum of the strain<br />

energies stored in each member due to bending, shear, torsion and axial<br />

loading.<br />

The use of this will be illustrated by considering a simply-supported beam of<br />

length l subject to an external loading (see Fig. 9.27). Strain energy stored in the<br />

beam is predominantly flexural and is given by<br />

l<br />

2 M dx<br />

Ú 2EI<br />

0<br />

x1= deflection under Pl=<br />

P<br />

∂ Ê<br />

Á<br />

∂ Ë<br />

∂M<br />

is the bending moment due to a unit load and is denoted by m.<br />

∂P1<br />

Hence the procedure of the unit load method can be outlined (see Fig. 9.27):<br />

El<br />

(9.21)<br />

M<br />

(1) diagram due to the external loading is obtained.<br />

EI<br />

(2) The external loads are now removed and the moment diagram (m) due to a<br />

unit load applied at the point of required deflection is drawn.<br />

(3) These two diagrams should now be integrated; in other words, the ordinates of<br />

the two diagrams are multiplied to obtain the deflection, given by<br />

l<br />

x<br />

M<br />

= Ú mdx EI<br />

0<br />

1<br />

l l<br />

2<br />

M dxˆ<br />

˜ =<br />

2EI<br />

¯<br />

Ú Ú<br />

M M<br />

EI P x<br />

∂<br />

d<br />

∂<br />

0 0 1

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