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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 />

320 Introduction to manual and computer analysis<br />

Fig. 9.31 Stress components on a plane element<br />

components. For the state of plane stress, the stress components are related to the<br />

strain components as given below:<br />

(9.25)<br />

where E and n are Young’s modulus and Poisson’s ratio respectively.<br />

The matrix [D] is referred to as the elasticity or property matrix. The strain energy<br />

of the element is given by Equation (9.22) as<br />

(9.26)<br />

Denoting the generalized nodal displacement by the vector {d e },<br />

(9.27)<br />

where {A} = [a1, a2, ...,an] T d<br />

, which is a vector of polynomial constants, and [C] is a<br />

transformation matrix.<br />

The strains are obtained through making appropriate differentiations of the<br />

displacement function with respect to the relevant co-ordinate variable x or y.<br />

Thus,<br />

e<br />

È<br />

s<br />

1 n 0˘<br />

Ï x ¸<br />

e x<br />

Ô Ô E<br />

Í ˙ Ï ¸<br />

Ìs<br />

y ˝ = Ín<br />

1 0˙<br />

Ô Ô<br />

e<br />

2<br />

Ì y ˝<br />

Ô<br />

t<br />

Ô 1 - n Í 1 - n ˙<br />

Ó xy ˛ Í0<br />

0 Ô<br />

g<br />

Ô<br />

xy<br />

Î 2 ˙ Ó ˛<br />

˚<br />

\{ s}= [ D]{}<br />

e<br />

1 T<br />

U = Ú Ú {} e [ D]{}<br />

e d( vol)<br />

2<br />

{ }= [ C]{ A}<br />

Ïe<br />

Ô<br />

{}= e Ìe<br />

Ô<br />

Óg<br />

x<br />

y<br />

xy<br />

Ï ∂u ∂x<br />

¸<br />

¸ Ô Ô<br />

Ô Ô ∂v ∂y<br />

Ô<br />

˝ = Ì ˝<br />

˛<br />

Ô Ô<br />

∂u<br />

∂v<br />

+ Ô<br />

Ô∂<br />

y ∂x<br />

Ô<br />

Ó ˛<br />

(9.28)

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