Page 87 - Handbook of Structural Steel Connection Design and Details
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Design of Connections for Axial, Moment, and Shear Forces

                    72    Chapter Two

                    of the gusset, the column, and the beam with axial forces only. Such a
                    set of forces is said to be “admissible.” But equilibrium is not the only
                    requirement that must be satisfied to establish the true distribution of
                    forces in a structure or connection. Two additional requirements are the
                    constitutive equations that relate forces to deformations and the com-
                    patibility equations that relate deformations to displacements.
                      If it is assumed that the structure and connection behave elastically
                    ( an assumption as to constitutive equations) and that the beam and the
                    column remain perpendicular to each other (an assumption as to defor-
                    mation–displacement equations), then an estimate of the moment in the
                    beam due to distortion of the frame (frame action) (Thornton, 1991) is
                    given by

                                                                  2
                                                             2
                                              P     I I c  sb 1 c d
                                                     b
                                      M   6
                                        D    Abc  I b  2I c   bc
                                                 a  1    b
                                                  b     c
                     where D   distortion
                           I   moment of inertia of beam   2370 in 4
                            b
                           I   moment of inertia of column   3840 in 4
                            c
                           P   brace force   855 kips
                           A   brace area   26.4 in 2
                           b   length of beam to inflection point (assumed at beam
                               midpoint)   175 in
                            c   length of columns to inflection points (assumed at column
                               midlengths)   96 in

                                      I
                         2I c          b
                    With     5 80 and   5 13.5
                          c           b
                                                             2
                                6 3 855 3 2370 3 3840     175 1 96 2
                      M                                              5 2670 kips-in
                        D   26.4 3 175 3 96 3 s13.5 1 80d s175 3 96d

                      This moment M is only an estimate of the actual moment that will
                                     D
                    exist between the beam and column. The actual moment will depend on
                    the strength of the beam-to-column connection. The strength of the
                    beam-to-column connection can be assessed by considering the forces
                    induced in the connection by the moment M as shown in Fig. 2.12. The
                                                            D
                    distortional force F is assumed to act as shown through the gusset
                                      D
                    edge connection centroids. If the brace force P is a tension, the angle
                    between the beam and column tends to decrease, compressing the gusset
                    between them, so F is a compression. If the brace force P is a com-
                                       D
                    pression, the angle between the beam and column tends to increase
                    and F is a tension. Figure 2.12 shows how the distortional force F is
                          D                                                       D


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