AISCAISC 360-22
Chapter E Design of members for compression

E7Members with slender elements

PDF page 116 · AISC 360-22

This section applies to slender-element compression members, as defined in Section B4.1 for elements in axial compression.

The nominal compressive strength, PnP_{n}, shall be the lowest value based on the applicable limit states of flexural buckling, torsional buckling, and flexural-torsional buckling in interaction with local buckling.

Pn=FnAeP_{n}=F_{n} A_{e}

(E7-1)

where

  • Ae=A_{e}= summation of the effective areas of the cross section based on reduced effective widths, be,deb_{e}, d_{e}, or heh_{e}, or the area as given by Equation E7-6 or E7-7, in. 2{ }^{2} (mm2)\left(\mathrm{mm}^{2}\right)
  • Fn= nominal stress determined in accordance with Section E3 or E4, ksi (MPa)  For single angles, determine Fn in accordance with Section E3 only. \begin{aligned} F_{n} & =\text { nominal stress determined in accordance with Section E3 or E4, ksi (MPa) } \\ & \text { For single angles, determine } F_{n} \text { in accordance with Section E3 only. }\end{aligned}

User Note: The effective area, AeA_{e}, may be determined by deducting from the gross area, AgA_{g}, the reduction in area of each slender element determined as (bbe)t\left(b-b_{e}\right) t.

E7.1 Slender Element Members Excluding Round HSS

The effective width, beb_{e} (for tees, this is ded_{e}; for webs, this is heh_{e} ), for slender elements is determined as follows:

(a) When λλrFyFn\lambda \leq \lambda_{r} \sqrt{\frac{F_{y}}{F_{n}}}

be=bb_{e}=b

(E7-2)

(b) When λ>λrFyFn\lambda>\lambda_{r} \sqrt{\frac{F_{y}}{F_{n}}}

be=b(1c1FelFn)FelFnb_{e}=b\left(1-c_{1} \sqrt{\frac{F_{e l}}{F_{n}}}\right) \sqrt{\frac{F_{e l}}{F_{n}}}

(E7-3)

where

  • bb \quad = width of the element (for tees this is dd; for webs this is hh ), in. (mm)
  • c1= effective width imperfection adjustment factor determined from Table E7.1 c2=114c12c1\begin{aligned} c_{1} & =\text { effective width imperfection adjustment factor determined from Table E7.1 } \\ c_{2} & =\frac{1-\sqrt{1-4 c_{1}}}{2 c_{1}} \end{aligned} (E7-4)

TABLE E7.1 Effective Width Imperfection Adjustment Factors, c1 and c2

CaseSlender Elementc1c2
(a)Stiffened elements except walls of square and rectangular HSS0.181.31
(b)Walls of square and rectangular HSS0.201.38
(c)All other elements0.221.49

λ\lambda \quad = width-to-thickness ratio for the element as defined in Section B4.1

λr=\lambda_{r}= limiting width-to-thickness ratio as defined in Table B4.1a

Fel=(c2κrλ)FyF_{e l}=\left(c_{2} \frac{\kappa_{r}}{\lambda}\right) F_{y}

(E7-5)

= elastic local buckling stress determined according to Equation E7-5 or an elastic local buckling analysis, ksi (MPa)

E7.2 Round HSS

The effective area, AeA_{e}, is determined as follows:

(a) When Dt0.11EFy\frac{D}{t} \leq 0.11 \frac{E}{F_{y}}

Ae=AgA_{e}=A_{g}

(E7-6)

(b) When 0.11EFy<Dt<0.45EFy0.11 \frac{E}{F_{y}}<\frac{D}{t}<0.45 \frac{E}{F_{y}}

Ae=[0.038EFy(D/t)+23]AgA_{e}=\left[\frac{0.038 E}{F_{y}(D / t)}+\frac{2}{3}\right] A_{g}

where

D=D= outside diameter of round HSS, in. (mm)

t=t \quad= thickness of wall, in. (mm)

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