Page 120 - Handbook of Civil Engineering Calculations, Second Edition
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STRUCTURAL STEEL DESIGN               1.103

                              earlier equations in this section. The
                              major axis is the one for which I is
                              maximum; the minor axis is the one
                              for which  I is minimum. The major
                              and minor axes are referred to collec-
                              tively as the principal axes.
                                With reference to the equation
                                                       2
                              given earlier, namely, I x    I x
 cos
                                    2
                              + I y
 sin 	 – P x y  sin 2	, the orienta-
                              tion of the principal axes relative to
                              the given x
 and y
 axes is found by
                              differentiating  I x  with respect to  	,
                              equating this derivative to zero, and
                              solving for  	 to obtain tan 2
                              2P x y  /(I y
 – I x
 ), Fig. 15.  FIGURE 10. Effective column lengths.
                                The following statements are
                              corollaries of this equation:
                              1. The principal axes through a given
                                point are mutually perpendicular,
                                since the two values of 	 that satis-
                                fy this equation differ by 90°.
                              2. The product of inertia of an area with respect to its principal axes is zero.
                              3. Conversely, if the product of inertia of an area with respect to two mutually perpendi-
                                cular axes is zero, these are principal axes.
                              4. An axis of symmetry is a principal axis, for the product of inertia of the area with re-
                                spect to this axis and one perpendicular thereto is zero.
                                Let A 1 and A 2 denote two areas, both of which have a radius of gyration r with respect
                              to a given axis. The radius of gyration of their composite area is found in this manner: I c
                                                          2
                                          2
                                               2
                                                                                             2
                                I 1 + I 2   A 1 r + A 2 r   (A 1 + A 2 )r . But A 1 + A 2   A c . Substituting gives I c   A w r ;
                              therefore, r c   r.
                                This result illustrates the following principle: If the radii of gyration of several areas
                              with respect to a given axis are all equal, the radius of gyration of their composite area
                              equals that of the individual areas.
                                                      2
                                                                                             2
                                The equation I x   I 0 +  Ak , when applied to a single area, becomes I x   I 0 + Ak .
                                         2
                                    2
                                                      2
                                                          2 0.5
                                              2
                              Then Ar x   Ar 0 + Ak , or r x   (r 0 + k ) . If the radius of gyration with respect to a cen-
                              troidal axis is known, the radius of gyration with respect to an axis parallel thereto may be
                              readily evaluated by applying this relationship.
                                The Euler equation for the strength of a slender column reveals that the member tends
                              to buckle about the minor centroidal axis of its cross section. Consequently, all column
                              design equations, both those for slender members and those for intermediate-length mem-
                              bers, relate the capacity of the column to its minimum radius of gyration. The first step in
                              the investigation of a column, therefore, consists in identifying the minor centroidal axis
                              and evaluating the corresponding radius of gyration.
                              CAPACITY OF A BUILT-UP COLUMN
                              A compression member consists of two C15   40 channels laced together and spaced
                              10 in. (254.0 mm) back to back with flanges outstanding, as shown in Fig. 11. What axial
                              load may this member carry if its effective length is 22 ft (6.7 m)?
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