AISCAISC 360-22
Formulas

Formulas: general provisions

PDF page 700 · AISC 360-22

Formula 1

The bracing requirements in Sections 6.2 and 6.3 generally are not sufficient to permit the development of member strengths based on LcL_{c} or LbL_{b} smaller than LbrL_{b r}; that is, the development of column or beam strengths based on a corresponding effective length factor of K<1K<1.

K<1K<1

Formula 2

The ideal bracing stiffness for this column associated with Lc=Lbr=LL_{c}=L_{b r}=L; that is, the bracing stiffness necessary to develop a column critical buckling load of Pcr=Pe=π2EI/Lbr2P_{c r}=P_{e}=\pi^{2} E I / L_{b r}^{2}, is Pb/LbrP_{b} / L_{b r}.

Lc=Lbr=LL_{c}=L_{b r}=L

Formula 3

Pcr=Pe=π2EI/Lbr2P_{c r}=P_{e}=\pi^{2} E I / L_{b r}^{2}

Formula 4

A brace having 5 times this stiffness is required for the column to reach a critical load of 95%95 \% of Pcr=π2EI/(0.7Lbr)2P_{c r}=\pi^{2} E I /\left(0.7 L_{b r}\right)^{2} based on Lc=0.7LbrL_{c}=0.7 L_{b r}.

Pcr=π2EI/(0.7Lbr)2P_{c r}=\pi^{2} E I /\left(0.7 L_{b r}\right)^{2}

Formula 5

Lc=0.7LbrL_{c}=0.7 L_{b r}

Formula 6

β=βi\beta = \beta_i — color: black; symbol: Solid line

β=βi\beta = \beta_i

Formula 7

Δo=0.002Lbr\Delta_o = 0.002L_{br} (text_label - position: x = 1.6, y = 0.3)

Δo=0.002Lbr\Delta_o = 0.002L_{br}

Formula 8

For columns, the value that is often used for the initial out-of-alignment, Δo=0.002Lbr\Delta_{o}=0.002 L_{b r}, equals the initial out-of-plumbness provided in the AISC Code of Standard Practice for Steel Buildings and Bridges (AISC, 2022a).

Δo=0.002Lbr\Delta_{o}=0.002 L_{b r}

Formula 9

In Figure C-A-6.3, for a brace stiffness of βbr=2βi\beta_{b r}=2 \beta_{i} and the initial imperfection of Δo=Lbr/500\Delta_{o}=L_{b r} / 500, the resulting brace force, PbrP_{b r}, for this point-bracing system is equal to 0.4%0.4 \% of PeP_{e} at P/Pe=1.0P / P_{e}=1.0.

βbr=2βi\beta_{b r}=2 \beta_{i}

Formula 10

Δo=Lbr/500\Delta_{o}=L_{b r} / 500

Formula 11

Similarly, for torsional bracing of beams, the important imperfection is an initial rotation, θo=Lbr/(500ho)\theta_{o}=L_{b r} /\left(500 h_{o}\right) (Wang and Helwig, 2005), where hoh_{o} is the distance between flange centroids.

θo=Lbr/(500ho)\theta_{o}=L_{b r} /\left(500 h_{o}\right)

Formula 12

For such cases, Chen and Tong (1994) recommend the use of an average initial displacement due to erection tolerances of Δo=Lbr/(500no)\Delta_{o}=L_{b r} /\left(500 \sqrt{n_{o}}\right), where non_{o} is the number of columns, each with a random Δo\Delta_{o}, stabilized by the bracing system.

Δo=Lbr/(500no)\Delta_{o}=L_{b r} /\left(500 \sqrt{n_{o}}\right)

Equation C-A-6-1

Vbr=V1st+2PrLbrΔo total V_{b r}=V_{1 s t}+2 \frac{P_{r}}{L_{b r}} \Delta_{o \text { total }}

where

  • Lbr= unbraced length within the panel under consideration, in. (mm) \begin{aligned} L_{b r} & =\text { unbraced length within the panel under consideration, in. (mm) }\end{aligned}
  • Pr= sum of the required axial forces in the columns being stabilized, kips (N) \begin{aligned} P_{r} & =\text { sum of the required axial forces in the columns being stabilized, kips (N) }\end{aligned}
  • V1st= first-order shear force in the bracing system due to gravity and/or lateral  loading on the structure, temperature effects, etc., kips (N) \begin{aligned} V_{1 s t} & =\text { first-order shear force in the bracing system due to gravity and/or lateral } \\ & \text { loading on the structure, temperature effects, etc., kips (N) }\end{aligned}

Δo,total =\Delta_{o \text {,total }}= total relative displacement between the ends of the unbraced length under consideration due to erection tolerances, first-order effects of gravity and/or lateral loads on the structure, and first-order effects (i.e., the effects prior to amplification from member axial compression) from any other sources such as temperature movement, connection slip, etc., in. (mm)

Equation C-A-6-3

Vbr=V1st+11βbr2βactPrLbrΔo. total V_{b r}=V_{1 s t}+\frac{1}{1-\frac{\beta_{b r}}{2 \beta_{a c t}}} \frac{P_{r}}{L_{b r}} \Delta_{o . \text { total }}

Equation C-A-6-4

1βact=1βconn +1βbrace \frac{1}{\beta_{a c t}}=\frac{1}{\beta_{\text {conn }}}+\frac{1}{\beta_{\text {brace }}}

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