The Design of Modern Steel Bridges - TEDI
The Design of Modern Steel Bridges - TEDI
The Design of Modern Steel Bridges - TEDI
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132 <strong>The</strong> <strong>Design</strong> <strong>of</strong> <strong>Modern</strong> <strong>Steel</strong> <strong>Bridges</strong><br />
in accordance with the Hencky–Mises yield criterion (i.e. equation (5.27) with<br />
tcr replaced by tl given above), and (ii) plastic hinges occur in the flanges,<br />
which together with the yielded zone WXYZ form a plastic mechanism.<br />
Considering the virtual work done in this mechanism and adding the resistance<br />
<strong>of</strong> the three stages, one obtains the ultimate shear capacity as<br />
Vu ¼ 4Mp<br />
c þ ctwst sin 2 yt þ stbtwðcot yt fÞ sin 2 yt þ t1btw ð5:32Þ<br />
where Mp is the plastic moment <strong>of</strong> resistance <strong>of</strong> the flange, c is the distance <strong>of</strong><br />
the internal plastic hinge (see Fig. 5.22) in one flange from the corner, and st is<br />
the membrane tensile stress, given by equation (5.27), with tl replacing tcr. <strong>The</strong> equilibrium condition <strong>of</strong> the flange between W and X (or between Z<br />
and Y) in Fig. 5.22 leads to<br />
c ¼ 2<br />
rffiffiffiffiffiffiffiffiffi<br />
Mp<br />
; but>j a<br />
sin yt sttw<br />
Putting this expression for c in equation (5.32) leads to the ultimate shear<br />
capacity tu being given by<br />
tu<br />
ty<br />
¼ t1<br />
ty<br />
tu<br />
ty<br />
rffiffiffiffi<br />
pffiffiffiffi<br />
st<br />
þ 5:264 sin yt m<br />
¼ t1<br />
ty<br />
þ 6:928m<br />
f<br />
ty<br />
þðcot yt fÞ sin 2 st<br />
yt<br />
ty<br />
st<br />
þ sin yt cos yt when m5<br />
ty<br />
f2 sin 2 ytst<br />
6:928ty<br />
when m4 f2 sin 2 ytst<br />
6:928ty<br />
ð5:33aÞ<br />
Figure 5.22 Tension-field mechanism <strong>of</strong> Porter, Rockey and Evans[8].<br />
ð5:33bÞ