SN001a (NCCI - Critical Axial Load for Torsional and Flexural Torsional Buckling Modes)

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  • 8/18/2019 SN001a (NCCI - Critical Axial Load for Torsional and Flexural Torsional Buckling Modes)

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      NCCI: Critical axial load for torsional and flexural torsional buckling modes

    SN001a-EN-EU

    NCCI: Crit ical axial load for torsional and flexural torsionalbuckling modes

    This NCCI gives the expressions for the critical axial load for the torsional buckling mode and the flexural-torsional buckling mode.

    Contents

    1. General 2

    2. Torsional buckling 2

    3. Flexural-torsional buckling 3

    4. References 4

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      NCCI: Critical axial load for torsional and flexural torsional buckling modes

    SN001a-EN-EU

    1. General

    For the following common cases, torsional and flexural torsional buckling will not give alower mode than flexural buckling :

      Doubly symmetric I and H sections (provided that both flanges are restrained at positionsof lateral restraint)

      Hollow sections

    However, in some particular cases, the torsional buckling mode or the flexural-torsional

     buckling mode of an axially loaded member may correspond to a critical load lower than the

    one corresponding to the flexural buckling mode, especially for open sections. This document

    gives rules to determine the critical load for such cases.

    This document deals with uniform members only and for which the conditions of restraint ateach end of the member are at least :

      restrained against lateral movement  restrained against rotation about the longitudinal axis

    2. Torsional buckling

    The critical axial load N cr.T for torsional buckling mode may be calculated from :

    ⎟⎟ ⎠

     ⎞⎜⎜⎝ 

    ⎛  +=2

    2

    2

    T

    wt

    o

    Tcr,

    1

    l

     EI GI 

    i N 

      π  

      (1)

    with:

    2

    o

    2

    o

    2

    z

    2

    y

    2

    o  z yiii   +++=   (2)

    where:

     E   is the Young modulus (E = 210000 N/mm2)

    G  is the shear modulus (G = 80770 N/mm2)

     I t  is the torsion constant

     I w  is the warping constant

    lT  is the buckling length regarding the torsional buckling mode. In general, lT should be

    taken as the system length, except when a special device prevents the warping at the

    ends of the member.

     yo and zo are the coordinates of the shear centre with respect to the centroid (see Figure 2.1).

    For a doubly symmetric cross-section, the shear centre coincides with the centroid;

    then yo = 0 and  zo = 0

    iy  is the radius of gyration of the cross-section about the strong axis

    iz  is the radius of gyration of the cross-section about the weak axis

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      NCCI: Critical axial load for torsional and flexural torsional buckling modes

    SN001a-EN-EU

    G

    S

     z

     y

     yo  zo 

     Figure 2.1  Coordinates of the shear centre S with respect to the centroid G

    3. Flexural-torsional buckling

    The flexural-torsional buckling mode should be considered only when the shear centre does

    not coincide with the centroid.

    The critical axial load N cr.TF for the flexural-torsional buckling mode is the smallest root of the

    following cubic equation in N  :

    ( )( )( ) ( )   ( ) 022222 =−−−−−−− ycr,ozcr,oTcr,zcr,ycr,  N  N  z N  N  N  y N  N  N  N  N  N  N io   (3)

    where

     N cr,y and N cr,z are the critical axial loads for flexural buckling about yy and zz axes

    respectively

     N cr.T  is the critical axial load for torsional buckling mode, see § 2.

    The equation may also be written as follows :

    ( )   ( ) 22232

     N  N  N  N  y N  z N i

     N i

    ii⎥⎦

    ⎤⎢⎣

    ⎡++−++

    ⎟⎟

     ⎠

     ⎞

    ⎜⎜

    ⎝ 

    ⎛    +Tcr,zcr,ycr,ozcr,oycr,2

    oo

    2

    z

    2

    y 1 

    0Tcr,zcr,ycr,ycr,Tcr,Tcr,zcr,zcr,ycr,   =−+++  N  N  N  N  N  N  N  N  N  N   

    (4)

    When the cross-section is symmetric about the y-y-axis (see Figure 3.1), the critical axial load

    may be obtained from :

    ( )  ( )

    ⎟⎟

     ⎠

     ⎞

    ⎜⎜

    ⎝ 

    ⎛    +−+−+

    +=

    2

    o

    2

    z

    2

    y

    Tcr,ycr,

    2

    Tcr,ycr,Tcr,ycr,2

    z

    2

    y

    2

    oTFcr,

    i

    ii N  N 4 N  N  N  N 

    ii2

    i N    (5)

    When the cross-section is symmetric about the z-z-axis, N cr.y should be replaced by N cr.z in theabove expression.

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      NCCI: Critical axial load for torsional and flexural torsional buckling modes

    SN001a-EN-EU

     yo 

    GS y y

     z

     z

     Figure 3.1 

    Cross-section symmetric about y-y-axis

    4. References

    1  Timoshenko, S.P. and Gere, J.M.

    Theory of elastic stability. 2nd 

     Edition. Mc Graw-Hill. 1961.

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      NCCI: Critical axial load for torsional and flexural torsional buckling modes

    SN001a-EN-EU

    Quality Record

    RESOURCE TITLE NCCI: Critical axial load for torsional and flexural torsional bucklingmodes

    Reference(s)

    ORIGINAL DOCUMENT

    Name Company Date

    Created by  A. BUREAU CTICM 02/02/05

    Technical content checked by Y. GALEA CTICM 02/02/05

    Editorial content checked by D C Iles SCI 2/3/05

    Technical content endorsed by thefollowing STEEL Partners:

    1. UK G W Owens SCI 1/3/05

    2. France  A Bureau CTICM 1/3/05

    3. Sweden  A Olsson SBI 1/3/05

    4. Germany C Mueller RWTH 1/3/05

    5. Spain J Chica Labein 1/3/05

    Resource approved by TechnicalCoordinator

    G W Owens SCI 21/04/06

    TRANSLATED DOCUMENT

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