NCCI: Elastic critical moment for lateral torsional buckling

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NCCI: Elastic critical moment for lateral torsional buckling This NCCI gives the expression of the elastic critical moment for doubly symmetric crosssections. Values of the factors involved in the calculation are given for common cases. For a beam under a uniformly distributed load with end moments or a concentrated load at mid-span with end moments, the values for the factors are given in graphs. Contents 1. General. ethod for doubly symmetric sections 3. C 1 and C factors 4 4. References 1 Page 1

1. General For doubly symmetric cross-sections, the elastic critical moment cr may be calculated by the method given in paragraph. For cases not covered by the method given in paragraph, the elastic critical moment may be determined by a buckling analysis of the beam provided that the calculation accounts for all the parameters liable to affect the value of cr : geometry of the cross-section warping rigidity position of the transverse loading with regard to the shear centre restraint conditions The LTBeam software is specific software for the calculation of the critical moment cr. It may be downloaded free of charge from the following web site: http://www.cticm.com. ethod for doubly symmetric sections The method given hereafter only applies to uniform straight members for which the crosssection is symmetric about the bending plane. The conditions of restraint at each end are at least : restrained against lateral movement restrained against rotation about the longitudinal axis The elastic critical moment may be calculated from the following formula derived from the buckling theory : EI k I w kl GI t cr C1 C g C kl kw I EI g (1) where E is the Young modulus (E = 10000 N/mm ) G is the shear modulus (G = 80770 N/mm ) I I t is the second moment of area about the weak axis is the torsion constant I w is the warping constant Page

L is the beam length between points which have lateral restraint k and k w are effective length factors g is the distance between the point of load application and the shear centre. Note : for doubly symmetric sections, the shear centre coincides with the centroid. C 1 and C are coefficients depending on the loading and end restraint conditions (see 3). The factor k refers to end rotation on plan. It is analogous to the ratio of the buckling length to the system length for a compression member. k should be taken as not less than 1,0 unless less than 1,0 can be justified. The factor k w refers to end warping. Unless special provision for warping fixity is made, k w should be taken as 1,0. In the general case g is positive for loads acting towards the shear centre from their point of application (Figure.1). F S S F g > 0 g < 0 Figure.1 Point of application of the transverse load Page 3

In the common case of normal support conditions at the ends (fork supports), k and k w are taken equal to 1. cr C 1 EI L I I w L GI EI t C g C g () When the bending moment diagram is linear along a segment of a member delimited by lateral restraints, or when the transverse load is applied in the shear centre, C g = 0. The latter expression should be simplified as follows : EI I L GI w t cr C1 (3) L I EI For doubly symmetric I-profiles, the warping constant I w may be calculated as follows : I w I h t 4 f (4) where h t f is the total depth of the cross-section is the flange thickness 3. C 1 and C factors 3.1 General The C 1 and C factors depend on various parameters : section properties, support conditions, moment diagram It can be demonstrated that the C 1 and C factors depend on the ratio : EI GI w t L (5) The values given in this document have been calculated with the assumption that = 0. This assumption leads to conservative values of C 1. Page 4

3. ember with end moments only The factor C 1 may be determined from Table 3.1 for a member with end moment loading. -1 +1 Figure 3.1 ember with end moments Table 3.1 Values of C 1 for end moment loading (for k = 1) C 1 +1,00 1,00 +0,75 1,14 +0,50 1,31 +0,5 1,5 0,00 1,77-0,5,05-0,50,33-0,75,57-1,00,55 Page 5

3.3 ember with transverse loading Table 3. gives values of C 1 and C for some cases of a member with transverse loading, Table 3. Values of factors C 1 and C for cases with transverse loading (for k = 1) Loading and support conditions Bending moment diagram C 1 C 1,17 0,454,578 1,554 1,348 0,630 1,683 1,645 Note : the critical moment cr is calculated for the section with the maximal moment along the member 3.4 ember with end moments and transverse loading For combined loading of end moments and transverse loads as shown in Figure 3., values of C 1 and C may be obtained from the curves given hereafter. Two cases are considered: Case a) end moments with a uniformly distributed load Case b) end moments with a concentrated load at mid-span The moment distribution may be defined using two parameters : is the ratio of end moments. By definition, is the maximum end moment, and so : -1 1 ( = 1 for a uniform moment) is the ratio of the moment due to transverse load to the maximum end moment Case a) ql 8 Page 6

Case b) FL 4 Sign convention for : > 0 < 0 if and the transverse load (q or F), each supposed acting alone, bend the beam in the same direction (e.g. as shown in the figure below) otherwise The values of C 1 and C have been determined for k = 1 and k w = 1. q F L (a) L (b) Figure 3. End moments with a transverse load Page 7

3.0 C1.5.0 1.5 1.4 0,4 0,3 0, 0,1 0 1.3 0,8 0,7 0,6 0,5 1. 1, 1 1,5 1.1 1.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 > 0 5.0 C 1 4.5-0,9-1 -1,1 4.0-0,8 3.5-0,7-0,6 3.0-0,5.5-0,3-0,4-1,.0 1.5 0-0,1-0, -1,3-1,4-1,5-1,6-1,7-1,8-1.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 < 0 Figure 3.3 End moments and uniformly distributed load Factor C 1 Page 8

0.5 C 0.4 0.3 1, 1,5 1 0,9 0,7 0,8 0. 0,3 0,5 0,4 0,6 0.1 0, 0,1 0.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 > 0.5 C -1,.0-1,1-1 1.5-0,8-0,9-1,3-1,5-1,4-1,6-1,7 1.0-1,8 - -0,7-0,6 0.5-0,5-0,4-0,3-0, -0,1 0.0-1 -0.8-0.6-0.4-0. 0 0. 0. 4 0.6 0.8 1 < 0 Figure 3.4 End moments and uniformly distributed load Factor C Page 9

3.0 C1.5.0 1.5 1.4 0,7 0,6 0,5 0,4 0,3 0, 0,1 0 1.3 1. 0,9 0,8 1 1, 1,5 1 C 1.1 0, 0,1 1.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 > 0 4.0 C1 3.5-1 -1,1-1, -0,9 3.0-0,7-0,8-0,6.5-0,5-0,4-1,3-0,3-1,4-0, -1,5.0 0-0,1-1,6-1,7-1,8-1.5 1.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 < 0 Figure 3.5 End moments and point load at mid-span Factor C 1 Page 10

0.5 C 0.4 1,5 1, 0.3 0,6 1 0,9 0,8 0,7 0,5 0. 0,4 0,3 0.1 0, 0,1 0.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 > 0.5 C.0-1, -1,4-1,6 1.5-1,3-1,5-1,7 - -1,8-1,1-1 1.0-0,9-0,8-0,7 0.5-0,6-0,5-0,4-0,3-0, -0,1 0.0-1 -0.8-0.6-0.4-0. 0 0. 0.4 0.6 0.8 1 < 0 Figure 3.6 End moments and point load at mid-span Factor C Page 11

4. References 1 ENV 1993-1-1 Eurocode 3 : Design of steel structures Part 1.1 : General rules and rules for buildings. European Committee for Standardisation. Timoshenko, S.P. and Gere, J.. Theory of elastic stability. nd Edition. c Graw-Hill. 1961. 3 Djalaly, H. Calcul de la résistance ultime au déversement dans le cas de la flexion déviée. Revue Construction étallique n 3-1974. CTIC. 4 Galéa, Y. Déversement élastique d une poutre à section bi-symétrique soumise à des moments d extrémité et une charge repartee ou concentrée. Revue Construction étallique n -00. CTIC. Page 1

Quality Record RESOURCE TITLE NCCI: Elastic critical moment for lateral torsional buckling Reference(s) ORIGINAL DOCUENT Name Company Date Created by Alain Bureau CTIC Technical content checked by Yvan Galéa CTIC Editorial content checked by D C Iles SCI /3/05 Technical content endorsed by the following STEEL Partners: 1. UK G W Owens SCI 1/3/05. France A Bureau CTIC 1/3/05 3. Sweden A Olsson SBI 1/3/05 4. Germany C ueller RWTH 1/3/05 5. Spain J Chica Labein 1/3/05 Resource approved by Technical Coordinator G W Owens SCI 1/4/06 TRANSLATED DOCUENT This Translation made and checked by: Translated resource approved by: Corrigendum 010-10-1: Figure 3.4 Labels corrected (for curves 1.1 to 1.9) Page 13

Wrapper Information Title* NCCI: Elastic critical moment for lateral torsional buckling Series Description* Access Level* This NCCI gives the expression of the elastic critical moment for doubly symmetric crosssections. Values of the factors involved in the calculation are given for common cases. For a beam under a uniformly distributed load with end moments or a concentrat Expertise Identifiers* Filename P:\CP\CP554\Finaliation\SN files\003\.doc Format Category* Resource Type Viewpoint icrosoft Office Word; 14 Pages; 1400kb; Non Contradictory Complementary Information Subject* Application Area(s) ulti-storey buildings; Dates Created Date 1/10/010 Last odified Date Checked Date Valid From Valid To 03/0/005 Language(s)* Contacts Author Checked By Approved by Editor Last odified By Alain Bureau, CTIC Yvan Galéa, CTIC Keywords* See Also Lateral Torsional Buckling Eurocode Reference Worked Example(s) Commentary Discussion Other Coverage National Applicability Special Instructions Page 14