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The Design of Modern Steel Bridges - TEDI

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emains flat until an elastic critical value <strong>of</strong> the loading is reached. Also, as in<br />

the case <strong>of</strong> plates, stiffened plates may <strong>of</strong>ten have substantial post-buckling<br />

strengths.<br />

5.5.1 Elastic critical buckling <strong>of</strong> stiffened panels<br />

Two basic methods are available for the analysis <strong>of</strong> elastic critical buckling <strong>of</strong><br />

ideally flat residual-stress-free stiffened plates. In the classical method, either<br />

(i) a differential equation <strong>of</strong> equilibrium is solved in general terms by assuming<br />

a deflected shape and then the boundary conditions are used to obtain a<br />

characteristic equation for the elastic critical buckling load, or (ii) a Fouriertype<br />

series representation is set up for the possible deformation mode consistent<br />

with the boundary conditions and then an energy or work approach is<br />

applied. <strong>The</strong> second method, i.e. the numerical or computer-based method, can<br />

tackle the complex problems; in this method a solution is formed in terms <strong>of</strong> a<br />

discrete number <strong>of</strong> unknowns located at many points in the stiffened plate.<br />

Thus a large-order matrix equation is formed, whose coefficients are given by<br />

the geometry <strong>of</strong> the stiffened plate and its loading conditions; the elastic<br />

critical buckling load is the value <strong>of</strong> the load at which the determinant <strong>of</strong> the<br />

coefficients is zero. <strong>The</strong> critical buckling load <strong>of</strong> a stiffened panel is generally<br />

expressed as<br />

scr ¼ k p2 D<br />

b 2 t<br />

where k is a buckling coefficient that depends on the geometry <strong>of</strong> the stiffened<br />

plate, the loading pattern and the boundary conditions, plus three relative<br />

rigidities <strong>of</strong> the stiffener, given by<br />

flexural: g ¼ EIs=bd<br />

torsional: y ¼ GJs =bd<br />

extensional: d ¼ As=bt<br />

Rolled Beam and Plate Girder <strong>Design</strong> 137<br />

and D is the flexural rigidity <strong>of</strong> the plate, equal to Et 3 =12ð1 m 2 Þ<br />

b ¼ spacing <strong>of</strong> the stiffeners<br />

t ¼ thickness <strong>of</strong> the plate<br />

I s ¼ is the second moment <strong>of</strong> area <strong>of</strong> the stiffener cross-section, with the width<br />

<strong>of</strong> the plate acting with it, about its centroidal plane parallel to the plate<br />

Js ¼ torsional constant <strong>of</strong> the stiffener cross-section<br />

A s ¼ area <strong>of</strong> the cross-section.<br />

Many solutions are available for a large range <strong>of</strong> stiffened panel geometries<br />

and loading types in References [10] and [11] for ‘open’-type stiffener crosssections<br />

(i.e. not ‘closed’- or box-type cross-sections) with negligible torsional<br />

rigidity.

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