10.04.2013 Views

The Design of Modern Steel Bridges - TEDI

The Design of Modern Steel Bridges - TEDI

The Design of Modern Steel Bridges - TEDI

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

148 <strong>The</strong> <strong>Design</strong> <strong>of</strong> <strong>Modern</strong> <strong>Steel</strong> <strong>Bridges</strong><br />

where<br />

s 1 ¼ applied longitudinal stress on the stiffener<br />

t ¼ shear stress in the web<br />

s 2 ¼ transverse stress in the web<br />

ks ¼ defined in Section 5.5.4.<br />

5.6 Restraint at supports<br />

<strong>The</strong> lateral buckling strength <strong>of</strong> beams has been derived in Section 5.3 on the<br />

assumption that its cross-section at the supports is restrained fully against any<br />

lateral deflection <strong>of</strong> its flanges. In reality the stiffeners at the support restraint<br />

to prevent twisting <strong>of</strong> the beam section is likely to be finite. Flint[12] has<br />

derived a reduction in the elastic critical bending strength scr <strong>of</strong> a perfect<br />

simply supported beam as<br />

scr<br />

¼<br />

scr<br />

4 GJ<br />

for a central concentrated load<br />

3 LeS<br />

¼ 2GJ for constant bending moment on the<br />

LeS whole length <strong>of</strong> the beam:<br />

where<br />

GJ ¼ torsional rigidity <strong>of</strong> the beam<br />

L e ¼ effective length <strong>of</strong> the beam<br />

S ¼ stiffness <strong>of</strong> the support against twisting <strong>of</strong> the beam section.<br />

<strong>The</strong> reduction s b in the limiting bending stress s b <strong>of</strong> the imperfect simply<br />

supported beam is, taking the worse <strong>of</strong> the above two cases<br />

sb<br />

sb<br />

¼ scr<br />

scr<br />

sb scr<br />

scr sb<br />

¼ 2GJ<br />

LeS<br />

sb scr<br />

scr sb<br />

If we decide to limit sb to n% <strong>of</strong>sb, then<br />

2GJ<br />

LeS<br />

sb scr<br />

4 0:01 n<br />

scr sb<br />

or<br />

S 5 200 GJ<br />

n Le<br />

sb scr<br />

scr sb<br />

ð5:45Þ<br />

From equations (5.7) and (5.8) in Section 5.3.1, assuming k, and the shape<br />

factor (i.e. the ratio <strong>of</strong> the plastic to elastic modulus) to be each approximately<br />

equal to unity, scr can be expressed as<br />

scr<br />

sy<br />

2 Le<br />

¼ p<br />

ry<br />

rffiffiffiffiffi 2<br />

sy<br />

E<br />

¼ 5700<br />

b 2

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!