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                                                       LATERAL-FORCE DESIGN


                                                                                   LATERAL-FORCE DESIGN  8.13

                      8.5 DYNAMIC METHOD OF SEISMIC LOAD DISTRIBUTION

                                  The equivalent static-force method (Art. 8.4) is based on a single-mode response with approximate
                                  load distributions and corrections for higher-mode response. These simplifications are appropriate
                                  for simple, regular structures. However, they do not consider the full range of seismic behavior in
                                  complex structures. The dynamic method of seismic analysis is required for many structures with
                                  unusual or irregular geometry, since it results in distributions of seismic design forces that are con-
                                  sistent with the distribution of mass and stiffness of the frames, rather than arbitrary and empirical
                                  rules. Irregular structures include frames with any of the following characteristics:
                                  • The lateral stiffness of any story is less than 70% of that of the story above or less than 80% of the
                                   average stiffness for the three stories above, that is, soft stories.
                                  • The mass of any story is more than 150% of the effective mass for an adjacent story, except for a
                                   light roof above.
                                  • The horizontal dimension of the lateral-force-resisting system in any story is more than 130% of
                                   that of an adjacent story.
                                  • The story strength is less than 80% of the story above.
                                  • The in-plane offset of the lateral-force-resisting elements is greater than the length of these elements.
                                    Frames with horizontal irregularities place great demands on floors acting as diaphragms and the
                                  horizontal load-distribution system. Special care is required in their design when any of the follow-
                                  ing conditions exist:
                                  • The maximum story drift due to torsional irregularity is more than 1.2 times the average story drift
                                   for the two ends of the structure.
                                  • There are reentrant corners in the plan of the structure with projections more than 15% of the plan
                                   dimension.
                                  • The diaphragms are discontinuous or have cutouts or openings totaling more than 50% of the
                                   enclosed area or changes in effective diaphragm stiffness of more than 50%.
                                  • There are discontinuities in the lateral-force load path.
                                    Irregular structures commonly require use of a variation of the dynamic method of seismic analy-
                                  sis, since it provides a more appropriate distribution of design loads. Many of these structures should
                                  also be subjected to a step-by-step dynamic analysis (linear or nonlinear) for specific accelerations
                                  to check the design further. Nonlinear pushover analyses are also used with increasing frequency to
                                  evaluate the inelastic behavior and inelastic seismic design in irregular or unusual structures.
                                    The dynamic method is based on equations of motion for linear-elastic seismic response. The
                                  equation of motion for a single-degree-of-freedom system subjected to a seismic ground accelera-
                                  tion a g may be expressed as

                                                                2
                                                               dx   dx
                                                             m    +  c  +  kx = − ma g                (8.13)
                                                               dt 2  dt
                                        2
                                           2
                                  where d x/dt is the acceleration of the structure, dx/dt is the velocity relative to the ground motion,
                                  and x is the displacement from an equilibrium position. The coefficients m, c, and k are the mass,
                                  damping, and stiffness of the system, respectively. Equation (8.13) can be solved by a number of
                                  methods.
                                    The maximum acceleration is often expressed as a function of the fundamental period of vibra-
                                  tion of the structure in a response spectrum. The response spectrum depends on the acceleration
                                  record. Since response varies considerably with acceleration records and structural period, smoothed
                                  response spectra are commonly used in design to account for the many uncertainties in future earth-
                                  quakes and actual structural characteristics.



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