AISCAISC 360-22
Chapter F Design of members for flexure

F4Other I-shaped members with compact or noncompact webs bent about their major axis

PDF page 124 · AISC 360-22

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

User Note: I-shaped members for which this section is applicable may be de- signed conservatively using Section F5.

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.

F4.1 Compression Flange Yielding

Mn=RpcMycM_{n}=R_{p c} M_{y c}

(F4-1)

where

Myc= yield moment in the compression flange, kip-in. (N-mm) =FySxc\begin{aligned} M_{y c} & =\text { yield moment in the compression flange, kip-in. (N-mm) } \\ & =F_{y} S_{x c}\end{aligned}

Rpc=R_{p c}= web plastification factor, determined in accordance with Section F4.2(c)(6)

Sxc=S_{x c}= elastic section modulus referred to compression flange, in. 3( mm3){ }^{3}\left(\mathrm{~mm}^{3}\right)

F4.2 Lateral-Torsional Buckling

(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}
Mn=CbRpcMyc(RpcMycFLSxc)(LbLpLrLp)RpcMycM_{n}=C_{b}\left|R_{p c} M_{y c}-\left(R_{p c} M_{y c}-F_{L} S_{x c}\right)\left(\frac{L_{b}-L_{p}}{L_{r}-L_{p}}\right)\right| \leq R_{p c} M_{y c}

(F4-2)

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

Mn=FcrSxcRpcMycM_{n}=F_{c r} S_{x c} \leq R_{p c} M_{y c}

(F4-3)

where

(1) MycM_{y c}, the yield moment in the compression flange, kip-in. (N-mm), is

Myc=FySxcM_{y c}=F_{y} S_{x c}

(F4-4)

(2) FcrF_{c r}, the critical stress, ksi (MPa), is

Fcr=Cbπ2E(Lb)21+0.078JSxcho(Lbrt)2F_{c r}=\frac{C_{b} \pi^{2} E}{\left(L_{b}\right)^{2}} \sqrt{1+0.078 \frac{J}{S_{x c} h_{o}}\left(\frac{L_{b}}{r_{t}}\right)^{2}}

(F4-5)

For IycIy0.23,J\frac{I_{y c}}{I_{y}} \leq 0.23, J shall be taken as zero,

where

Iyc= moment of inertia of the compression flange about the y-axis, in. 4(mm4)\begin{aligned} I_{y c} & =\text { moment of inertia of the compression flange about the } y\text {-axis, in. }^{4} \\ & \left(\mathrm{mm}^{4}\right)\end{aligned}

  • (3) FLF_{L}, nominal compression flange stress above which the inelastic buckling limit states apply, ksi (MPa), is determined as follows:

(i) When SxtSxc0.7\frac{S_{x t}}{S_{x c}} \geq 0.7

FL=0.7FyF_{L}=0.7 F_{y}

(F4-6a)

(ii) When SxtSxc<0.7\frac{S_{x t}}{S_{x c}}<0.7

FL=FySxtSxc0.5FyF_{L}=F_{y} \frac{S_{x t}}{S_{x c}} \geq 0.5 F_{y}

where

Sxt=S_{x t}= elastic section modulus referred to tension flange, in. 3( mm3){ }^{3}\left(\mathrm{~mm}^{3}\right)

  • (4) LpL_{p}, the limiting laterally unbraced length for the limit state of yielding, in. (mm), is
Lp=1.1rtEFyL_{p}=1.1 r_{t} \sqrt{\frac{E}{F_{y}}}

(F4-7)

  • (5) LrL_{r}, the limiting unbraced length for the limit state of inelastic lateral-torsional buckling, in. (mm), is
Lr=1.95ntEFLJSxcho+(JSxcho)2+6.76(FLE)2L_{r}=1.95 n_{t} \frac{E}{F_{L}} \sqrt{\frac{J}{S_{x c} h_{o}}}+\sqrt{\left(\frac{J}{S_{x c} h_{o}}\right)^{2}+6.76\left(\frac{F_{L}}{E}\right)^{2}}
  • (6) RpcR_{p c}, the web plastification factor, is determined as follows:

(i) When Iyc/Iy>0.23I_{y c} / I_{y}>0.23

(a) When hctw\frac{h_{c}}{t_{w}}

Rpc=MpMycR_{p c}=\frac{M_{p}}{M_{y c}}

(F4-9a)

(b) When hctw>λpw\frac{h_{c}}{t_{w}}>\lambda_{p w}

Mp Mp 2-p My Re Rpc M ус Myc w-pw Myc (F4-9b)

(ii) When Iyc/Iy0.23I_{y c} / I_{y} \leq 0.23

Rpc=1.0R_{p c}=1.0

(F4-10)

where

Mp=FyZx1.6FySxM_{p}=F_{y} Z_{x} \leq 1.6 F_{y} S_{x}

hc=h_{c}= twice the distance from the centroid to the following: the inside face of the compression flange less the fillet or corner radius, for rolled shapes; the nearest line of fasteners at the compression flange or the inside face of the compression flange when welds are used, for built-up sections, in. (mm)

λ

hch_{c}

trt_{\mathrm{r}}

tw

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

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

  • (7) rtr_{t}, the effective radius of gyration for lateral-torsional buckling, in. (mm), is determined as follows:
  • (i) For I-shapes with a rectangular compression flange
rt=bfc12(1+1aw)r_{t}=\frac{b_{f c}}{\sqrt{12\left(1+\frac{1}{a_{w}}\right)}}

(F4-11)

where

aw=hctwbfctfca_{w}=\frac{h_{c} t_{w}}{b_{f c} t_{f c}}

(F4-12)

bfc=b_{f c}= width of compression flange, in. (mm)

tfc=t_{f c}= thickness of compression flange, in. (mm)

tw=t_{w}= thickness of web, in. (mm)

  • (ii) For I-shapes with a channel cap or a cover plate attached to the compression flange
  • rt=r_{t}= radius of gyration of the flange components in flexural compression plus one-third of the web area in compression due to application of major-axis bending moment alone, in. (mm)

F4.3 Compression Flange Local Buckling

(a) For sections with compact flanges, the limit state of local buckling does not apply.

  • (b) For sections with noncompact flanges
Mn=RpcMyc(RpcMycFLSxc)(κκpfλrfλpf)M_{n}=R_{p c} M_{y c}-\left(R_{p c} M_{y c}-F_{L} S_{x c}\right)\left(\frac{\kappa-\kappa_{p f}}{\lambda_{r f}-\lambda_{p f}}\right)

(F4-13)

(c) For sections with slender flanges

Mn=0.9EkcSxcλ2M_{n}=\frac{0.9 E k_{c} S_{x c}}{\lambda^{2}}

(F4-14)

where

FL is defined in Equations F4-6a and F4-6b Rpc is the web plastification factor, determined by Equation F4-9a, F4-9b, or F4-10 kc=4h/tw and shall not be taken as less than 0.35 nor greater than 0.76 for cal-  culation purposes λ=bfc2tfc\begin{aligned} F_{L} & \text { is defined in Equations F4-6a and F4-6b } \\ R_{p c} & \text { is the web plastification factor, determined by Equation F4-9a, F4-9b, or F4-10 } \\ 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 cal- } \\ & \text { culation 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

F4.4 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=RptMytM_{n}=R_{p t} M_{y t}

(F4-15)

where

Myt= yield moment in the tension flange, kip-in. (N-mm) =FySxt\begin{aligned} M_{y t} & =\text { yield moment in the tension flange, kip-in. (N-mm) } \\ & =F_{y} S_{x t}\end{aligned}

RptR_{p t}, the web plastification factor corresponding to the tension flange yielding limit state, is determined as follows:

(1) When Iyc/Iy>0.23I_{y c} / I_{y}>0.23

(i) When hc pw tw

Rpt=MpMytR_{p t}=\frac{M_{p}}{M_{y t}}

(F4-16a)

(ii) When hctw>λpw\frac{h_{c}}{t_{w}}>\lambda_{p w}

Rpt=MpMyt(MpMyt1)(λλpwλrwλpw)MpMytR_{p t}=\left|\frac{M_{p}}{M_{y t}}-\left(\frac{M_{p}}{M_{y t}}-1\right)\left(\frac{\lambda-\lambda_{p w}}{\lambda_{r w}-\lambda_{p w}}\right)\right| \leq \frac{M_{p}}{M_{y t}}

(2) When Iyc/Iy0.23I_{y c} / I_{y} \leq 0.23

Rpt=1.0R_{p t}=1.0

(F4-17)

where

Mp=FyZx1.6FySxM_{p}=F_{y} Z_{x} \leq 1.6 F_{y} S_{x}

λ=htw\lambda=\frac{h}{t_{w}}

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

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

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