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AISC LRFD 1.pdf

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Comm. C1.] SECOND ORDER EFFECTS 187TABLE C-C1.1Amplification Factors and C mCase C m0 1.0Pu0.4 1− 04 .Pe1Pu0.4 1− 04 .Pe1Pu0.2 1− 0.2Pe1Pu0.3 1− 0.3Pe1Pu0.2 1− 0.2Pe1Galambos (1961) it was pointed out that Equation C1-3 could be used for in-planesecond order moments if the 0.4 limit was eliminated. Unfortunately, Austin (1961)was misinterpreted and a lateral-torsional buckling solution was used for anin-plane second-order analysis. This oversight has now been corrected.For beam columns with transverse loadings, the second-order moment can beapproximated by using the following equationC = + ψ P / Pm 1 u e1for simply supported memberswhereψ = π2δo EI1MoL− 2 o = maximum deflection due to transverse loading, in. (mm)M o = maximum factored design moment between supports due to transverseloading, kip-in. (N-mm)For restrained ends, some limiting cases are given in Table C-C1.1 together withtwo cases of simply supported beam-columns (Iwankiw, 1984). These values of C mare always used with the maximum moment in the member. For the restrained-end<strong>LRFD</strong> Specification for Structural Steel Buildings, December 27, 1999AMERICAN INSTITUTE OF STEEL CONSTRUCTION

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