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<strong>The</strong> 5th Cross-strait Conference on Structural and Geotechnical Engineering (SGE-5)<br />

<strong>Hong</strong> <strong>Kong</strong>, China, 13-15 July 2011<br />

FINITE ELEMENT STUDY OF INELASTIC LOCAL WEB BUCKLING CAPACITY<br />

OF COPED STEEL I-BEAM<br />

Y. Qin 1 , C. C. Lam 2 , V. P. Iu 3 , and K. P. Kou 4<br />

1,2,3,4 Department of Civil and Environmental Engineering,<br />

<strong>University</strong> of Macau, Macau SAR, China.<br />

2 Email: fstccl@umac.mo<br />

ABSTRACT<br />

In steel construction, beams often have to be coped at the flange to provide clearance for the framing beams or<br />

to maintain the main beam and the secondary beam at the same level. When the beams are coped, the local web<br />

buckling capacity of the beams at the coped region may be reduced. Depending on the cope details, the local<br />

web buckling capacity can be classified as elastic and inelastic web buckling. For coped beam with relatively<br />

short coped length and depth, part or the whole section of the web may yield before local web buckling occurs.<br />

In this paper, non-linear finite element analyze, which included both material and geometric nonlinearities, of<br />

the inelastic local web buckling capacity of coped steel I-beam is presented. <strong>The</strong> effects of different parameters,<br />

such as (1) web slenderness (d/t w ), (2) cope depth to beam depth ratio (d c /D), (3) cope length to reduced web<br />

depth ratio (c/h o ) and (4) initial imperfection of web section, to the web buckling capacity of coped steel I-beam<br />

were studied. <strong>The</strong> current finite element results showed that local web buckling capacity decreased with<br />

increased initial imperfection. Meanwhile, for beams with the smallest beam depth to web thickness ratio, both<br />

shear yielding capacity and elastic web buckling capacity gave conservative prediction when c/h o is larger than<br />

0.5. On the other hand, for beams with largest beam depth to web thickness ratio, the predicted elastic web<br />

buckling capacity was closed to the finite element results for c/h o larger than 0.75. However, the prediction of<br />

both shear yielding capacity and elastic web buckling capacity gave conservative prediction when c/h o is smaller<br />

than 0.75 for most of the cases in this study.<br />

KEYWORDS<br />

Cope beam; finite element method; inelastic analysis; local web buckling; steel structures.<br />

INTRODUCTION<br />

In order to make the beam flanges at the same elevation, in practical steel construction, beam flanges often have to<br />

be cut away from the major part to provide enough clearance for supports. <strong>The</strong> cope can be at the top (as shown in<br />

Figure 1), the bottom, or both flanges in combination. As a result, due to the coped flanges, the corresponding<br />

lateral-torsional buckling capacity and the local web buckling (LWB) capacity of the beam may be reduced. For<br />

the beams with lateral support, block shear failure of the connection at beam end and local web buckling were two<br />

potential failure modes. For thin webs, failure could occur by local web buckling at the coped region. <strong>The</strong> global<br />

lateral-torsional buckling behavior and the elastic local web buckling strength of coped steel-I beam were studied<br />

both experimentally and analytically by Cheng et al. (1984). Further studies of the design and behavior of coped I<br />

beams were also conducted by some researchers (Cheng and Yura 1986; Lam et al. 2000; Yam et al. 2000; Johan<br />

Maljaars et al. 2002; Yam et al. 2007). Based on the experimental and numerical investigations of the local web<br />

buckling strength of coped section, Yam et al. (2003) proposed a modified plate buckling equation that considered<br />

the shear buckling phenomenon for predicting the elastic local web buckling capacity of coped steel I-beam. It is<br />

proposed that the critical elastic web buckling reaction (R cr ) can be predicted by Eqs. (1) to (3).<br />

k<br />

s<br />

b<br />

0<br />

,<br />

⎛ h ⎞<br />

= a⎜<br />

⎟<br />

⎝ c ⎠<br />

R<br />

cr<br />

=τ t D − d )<br />

(1)<br />

cr<br />

w ( c<br />

2<br />

2<br />

π E ⎛ tw<br />

⎞<br />

τ = k<br />

2<br />

12( 1 )<br />

⎜<br />

⎟<br />

(2)<br />

cr s<br />

−υ<br />

⎝ h0<br />

⎠<br />

2<br />

d<br />

c<br />

a = 1.38<br />

−1.79<br />

,<br />

⎛ dc ⎞ ⎛ dc<br />

⎞<br />

b = 3.64⎜<br />

⎟ − 3.36⎜<br />

⎟ + 1. 55<br />

(3)<br />

D ⎝ D ⎠ ⎝ D ⎠<br />

-464-

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