49-34 The Civil Engineering Handbook, Second Edition
Torsional Flexural Buckling
Theoretical Basis
Apart from local buckling, perhaps the major difference in
behavior between hot-rolled steel and cold-formed steel struc-
tural members is to be found in the relative susceptibility of
the latter to torsional flexural buckling. Designers in hot-rolled
steel do not come across this phenomenon to a great extent,
partly because hot-rolled steel sections are generally thicker
and more compact than cold-formed steel sections, but more
generally because of the greater variety of sectional shapes that
are designed in cold-formed steel. When dealing with mem-
bers that are of arbitrary cross-section, a more general theo-
retical approach must be adopted than that used in the earlier
sections of this chapter.
Consider a member having a generally unsymmetrical cross
section, as depicted in Fig. 49.33. If this member is loaded in
compression, it is not possible to determine by inspection the direction in which the cross-section will
move during buckling. For such a cross section, on the basis of classical theory, which is detailed in
Murray (1984) and Allen and Bulson (1980), the deflections of the member will have components in the
x and y directions and twisting will also occur about the shear center, or center of twist. Indeed, if precise
analysis of the situation were to be carried out, it would be found that distortion, or change in shape of
the cross-section, is also a distinct possibility in thin-walled sections, but this complicates the analysis
considerably.
The application of classical theory to deal with cold-formed steel sections has been researched exten-
sively at Cornell University in the U.S. (Chajes and Winter, 1965; Peköz and Celebi, 1969), and Yu (1991)
gives a thorough summary of the design approach based on this work. If we consider that the section of
Fig. 49.33 is loaded through its centroid, and axes x-x and y-y are the principal axes, then the buckling
load, which in the general case is due to a combination of biaxial flexure and twisting, and thus denoted
P
TF
, may be obtained from the following equation:
(49.36)
In this equation I
c
is the polar second moment of area with respect to the shear center of the section;
P
EX
and P
EY
are the critical loads for buckling about the x and y axes, respectively; and P
T
is the torsional
buckling load. The dimensions x
o
and y
o
are the distances between the centroid of the section and its
shear center measured in the x and y directions, respectively. The smallest root of the equation gives the
value of P
TF
of interest, and this is always less than or equal to the smallest value of the individual critical
loads.
If the member has simple support conditions, as normally defined, at its ends, then P
EX
and P
EY
are
simply the Euler loads for buckling about the x-x and y-y axes, respectively. The torsional buckling load,
P
T
, however, is not fully described by the commonly accepted simple support conditions; closer exami-
nation of the support conditions must be carried out to define this load.
P
T
is defined by the following equation:
(49.37)
where G = the shear modulus for the material
J = the torsion constant for the section
FIGURE 49.33 Generally unsymmetrical
cross-section.