AISCAISC 360-22
Chapter F Design of members for flexure

F5Doubly symmetric and singly symmetric I-shaped members with slender webs bent about their major axis

PDF page 128 · AISC 360-22

This section applies to doubly symmetric and singly symmetric I-shaped members with slender webs attached to the mid-width of the flanges and bent about their major axis as defined in Section B4.1 for flexure.

The nominal flexural strength, MnM_{n}, shall be the lowest value obtained according to the limit states of compression flange yielding, lateral-torsional buckling, compression flange local buckling, and tension flange yielding.

F5.1 Compression Flange Yielding

Mp=RpgFySxcM_{p}=R_{p g} F_{y} S_{x c}

(F5-1)

F5.2 Lateral-Torsional Buckling

Mn=RpgFcrSxcM_{n}=R_{p g} F_{c r} S_{x c}

(F5-2)

(a) When LbLpL_{b} \leq L_{p}, the limit state of lateral-torsional buckling does not apply.

  • (b) When Lp<LbLrL_{p}<L_{b} \leq L_{r}
Fcr=CbFy(0.3Fy)(LbLpLrLp)FyF_{c r}=C_{b}\left|F_{y}-\left(0.3 F_{y}\right)\left(\frac{L_{b}-L_{p}}{L_{r}-L_{p}}\right)\right| \leq F_{y}

(c) When Lb>LrL_{b}>L_{r}

Сьп²Е For SF (F5-4) L

rt

where

LpL_{p} is defined by Equation F4-7

Lr=πrtE0.7FyL_{r}=\pi r_{t} \sqrt{\frac{E}{0.7 F_{y}}}

(F5-5)

rt = effective radius of gyration for lateral-torsional buckling as defined in Section F4, in. (mm)

RpgR_{p g}, the bending strength reduction factor, is

Rpg=1aw1,200+300aw(hc5.7twEFy)1.0R_{p g}=1-\frac{a_{w}}{1,200+300 a_{w}}\left(\frac{h_{c}-5.7}{t_{w}} \sqrt{\frac{E}{F_{y}}}\right) \leq 1.0

(F5-6)

awa_{w} is defined by Equation F4-12, but shall not exceed 10

F5.3 Compression Flange Local Buckling

Mn=RpgFcrSxcM_{n}=R_{p g} F_{c r} S_{x c}

(F5-7)

  • (a) For sections with compact flanges, the limit state of compression flange local buckling does not apply.
  • (b) For sections with noncompact flanges
Fcr=Fy(0.3Fy)(λλpfλrfλpf)F_{c r}=F_{y}-\left(0.3 F_{y}\right)\left(\frac{\lambda-\lambda_{p f}}{\lambda_{r f}-\lambda_{p f}}\right)

(F5-8)

(c) For sections with slender flanges

Fcr=0.9Ekc(bf2tf)2F_{c r}=\frac{0.9 E k_{c}}{\left(\frac{b_{f}}{2 t_{f}}\right)^{2}}

(F5-9)

where

kc=4h/tw and shall not be taken as less than 0.35 nor greater than 0.76 for calculation purposes λ=bfc2tfc\begin{aligned} k_{c} & =\frac{4}{\sqrt{h / t_{w}}} \text { and shall not be taken as less than } 0.35 \text { nor greater than } 0.76 \text { for calculation purposes } \\ \lambda & =\frac{b_{f c}}{2 t_{f c}}\end{aligned}

λpf=λp\lambda_{p f}=\lambda_{p}, the limiting width-to-thickness ratio for a compact flange as defined in Table B4.1b

λrf=λr\lambda_{r f}=\lambda_{r}, the limiting width-to-thickness ratio for a noncompact flange as defined in Table B4.1b

F5.4 Tension Flange Yielding

(a) When SxtSxcS_{x t} \geq S_{x c}, the limit state of tension flange yielding does not apply.

(b) When Sxt<SxcS_{x t}<S_{x c}

Mn=FySxtM_{n}=F_{y} S_{x t}

(F5-10)

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