AISCAISC 360-22
Formulas

Formulas: effective length method

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Formula 1

The effective length, Lc=KLL_{c}=K L, for column buckling based upon elastic or inelastic stability theory, or alternatively the equivalent elastic column buckling stress, Fe=π2E/(Lc/r)2F_{e}=\pi^{2} E /\left(L_{c} / r\right)^{2}, is used to calculate an axial compressive strength, PcP_{c}, through an empirical column curve that accounts for geom

Lc=KLL_{c}=K L

Formula 2

The effective length, Lc=KLL_{c}=K L, for column buckling based upon elastic or inelastic stability theory, or alternatively the equivalent elastic column buckling stress, Fe=π2E/(Lc/r)2F_{e}=\pi^{2} E /\left(L_{c} / r\right)^{2}, is used to calculate an axial compressive strength, PcP_{c}, through an empirical column curve that accounts for geometric imperfections and distributed yielding including the effects of residual stresses.

Fe=π2E/(Lc/r)2F_{e}=\pi^{2} E /\left(L_{c} / r\right)^{2}

Formula 3

If K<1.0K<1.0 is used for the calculation of the nominal compressive strength, PnP_{n}, in braced frames, the additional demands on the stability bracing systems and the influence on the second-order moments in beams providing restraint to the columns must be considered.

K<1.0K<1.0

Equation C-A-7-2

The alignment chart for sidesway uninhibited frames shown in Figure C-A-7.2 is based on the following equation:

GAGB(π/K)2366(GA+GB)(π/K)tan(π/K)=0\frac{G_{A} G_{B}(\pi / K)^{2}-36}{6\left(G_{A}+G_{B}\right)}-\frac{(\pi / K)}{\tan (\pi / K)}=0

Equation C-A-7-3

G=Σ(EcolIcol/Lcol)Σ(EgIg/Lg)=Σ(EI/L)colΣ(EI/L)gG=\frac{\Sigma\left(E_{c o l} I_{c o l} / L_{c o l}\right)}{\Sigma\left(E_{g} I_{g} / L_{g}\right)}=\frac{\Sigma\left(E I / L\right)_{c o l}}{\Sigma(E I / L)_{g}}

Equation C-A-7-4

Lg=Lg(2MF/MN)L_{g}^{\prime}=L_{g}\left(2-M_{F} / M_{N}\right)

Equation C-A-7-5

K2=Pstory RMPr(π2EIL2)(ΔHHL)π2EIL2(ΔH1.7Hcol L)K_{2}=\sqrt{\frac{P_{\text {story }}}{R_{M} P_{r}}\left(\frac{\pi^{2} E I}{L^{2}}\right)\left(\frac{\Delta_{H}}{H L}\right)} \geq \sqrt{\frac{\pi^{2} E I}{L^{2}}\left(\frac{\Delta_{H}}{1.7 H_{\text {col }} L}\right)}

Equation C-A-7-6

RM=10.15(Pmf/Pstory )R_{M}=1-0.15\left(P_{m f} / P_{\text {story }}\right)

where

Pmf,Pstory P_{m f}, P_{\text {story }}, and HH are as defined in Appendix 8, Section 8.1.3.

Equation C-A-7-7

Pe2=(HLΔH)PrPstory RM1.7HcolL/ΔHP_{e 2}=\left(\frac{H L}{\Delta_{H}}\right) \frac{P_{r}}{P_{\text {story }}} R_{M} \leq 1.7 H_{c o l} L / \Delta_{H}

Equation C-A-7-8

K2=π2EIL2Pstory Prπ2EI(Kn2L)258Kn2K_{2}=\sqrt{\frac{\pi^{2} E I}{L^{2}} \frac{P_{\text {story }}}{P_{r}} \sum \frac{\pi^{2} E I}{\left(K_{n 2} L\right)^{2}}} \geq \sqrt{\frac{5}{8}} K_{n 2}

where

Kn2K_{n 2} is defined as the value of KK determined directly from the alignment chart in Figure C-A-7.2.

Equation C-A-7-9

Pe2=(PrPstory )π2EI(Kn2L)21.6π2EI(Kn2L)2P_{e 2}=\left(\frac{P_{r}}{P_{\text {story }}}\right) \sum \frac{\pi^{2} E I}{\left(K_{n 2} L\right)^{2}} \leq 1.6 \frac{\pi^{2} E I}{\left(K_{n 2} L\right)^{2}}

Equation C-A-7-10

K2=1+(1M1M2)41+56(Pstory PmfPmf)K_{2}=\left|1+\left(1-\frac{M_{1}}{M_{2}}\right)^{4}\right| \sqrt{1+\frac{5}{6}\left(\frac{P_{\text {story }}-P_{m f}}{P_{m f}}\right)}

Equation C-A-7-11

In this equation, M1M_{1} and M2M_{2} are the smaller and larger end moments, respectively, in the column. These moments are determined from a first-order analysis of the frame under lateral load. Column inelasticity is considered in the derivation of this equation. The unconservative error in PcP_{c}, when it is based on K2K_{2} determined from Equation C-A-7-10, is less than 3%3 \% if the following inequality is satisfied:

(ΣPymfHL/ΔH)(Pstory Pmf)0.45\left(\frac{\Sigma P_{y m f}}{H L / \Delta_{H}}\right)\left(\frac{P_{\text {story }}}{P_{m f}}\right) \leq 0.45

where

ΣPymf\Sigma P_{y m f} is the sum of the axial yield strengths of all columns in the story that are part of moment frames, if any, in the direction of translation being considered.

Formula 14

For slender columns, the calculation of the effective length, Lc=KLL_{\mathrm{c}}=K L, and PnKLP_{n K L} is critical to achieving an accurate solution when using the effective length method.

Lc=KLL_{\mathrm{c}}=K L

Found in

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