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Timothy A. Philpot - Mechanics of materials _ an integrated learning system-John Wiley (2017)

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674

COLuMNS

70

60

σ

Y =

50

=

σ cr

40

30

σ

Y =

=

20

10

0

0 50 100 150 200

FIGURE 16.5 Graphs of Euler buckling stress for steel and an

aluminum alloy.

L—

Equation (16.8) is valid only when the critical stress is less than the proportional limit for

the material, because the derivation of that equation is based on Hooke’s law. Therefore, a

horizontal line is drawn on the graph at the 36 ksi proportional limit stress for the structural

steel and at the 60 ksi proportional limit for the aluminum alloy, and the respective Euler

stress curves are truncated at these values.

Implications of Euler Buckling

An examination of Equations (16.5) and (16.8) reveals several implications for the buckling

of an ideal column:

• The Euler buckling load is inversely related to the square of the column length. Therefore,

the load that causes buckling decreases rapidly as the column length increases.

• The only material property that appears in Equations (16.5) and (16.8) is the elastic

modulus E, which represents the stiffness of the material. One means of increasing the

load-carrying capacity of a given column is to use a material with a higher value of E.

• Buckling occurs about the cross-sectional axis that corresponds to the minimum moment

of inertia (which in turn corresponds to the minimum radius of gyration). Therefore, it

is generally inefficient to select a member that has great disparity between the maximum

and minimum moments of inertia for use as a column. This inefficiency can be

mitigated if additional lateral bracing is provided to restrain lateral deflection about the

weaker axis.

• Since the Euler buckling load is directly related to the moment of inertia I of the cross

section, a column’s load-carrying capacity can often be improved, without increasing

its cross-sectional area, by employing thin-walled tubular shapes. Circular pipes and

square hollow structural sections are particularly efficient in this regard. The radius

of gyration r defined in Equation (16.7) provides a good measure of the relationship

between moment of inertia and cross-sectional area. In choosing between two shapes

of equal area for use as a column, it is helpful to keep in mind that the shape with the

larger radius of gyration will be able to withstand more load before buckling.

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