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University of California, Berkeley |
Note: this paper was presented at the EERC-CUREe Symposium in Honor of Vitelmo V. Bertero, January 31 - February 1, 1997, Berkeley, California.

where [F subscript y (mu = 1)] is the lateral yielding strength required to maintain the system elastic; [F subscript y (mu = mu subscript i) is the lateral yielding strength required to maintain the displacement ductility demand [mu] less or equal to a predetermined maximum tolerable displacement ductility ratio [mu subscript i].
In general, for structures allowed to respond nonlinearly during earthquakes ground motions, inelastic deformations increase as the lateral yielding strength of the structure decreases (or as the design reduction factor increases). For a given ground motion and a maximum tolerable displacement ductility demand [mu subscript i], the problem is to compute the minimum lateral strength capacity [F subscript y (mu = mu subscript i)] that has to be supplied to the structure in order to avoid ductility demands larger than [mu subscript i]. Alternatively, for a given elastic design spectrum, the problem is to compute the maximum strength reduction factor that can be used in order to avoid ductility demands larger than [mu subscript i].
For design purposes, [R subscript mu] corresponds to the maximum reduction in strength that can be used in order to limit the displacement ductility demand to a maximum tolerable ductility demand [mu subscript i] in a single-degree-of-freedom (SDOF) system that will have a lateral strength equal to the design strength.
For a given ground motion, computation of [F subscript y (mu = mu subscript i)] involves iteration, for each period and for each target (i.e., maximum tolerable) ductility ratio, on the lateral strength [F subscript y] until the computed ductility demand [mu] is, within a certain tolerance, the same as the target ductility ratio [mu subscript i]. For a given ground acceleration time history, a [R subscript mu] spectrum can be constructed by plotting the strength reduction factors (computed with Eq. 1) of a family of SDOF systems (with different periods of vibrations) undergoing different levels of inelastic deformation [mu subscript i] when subjected to the same ground motion.

Miranda and Bertero (1994) recently summarized the results of 13 different studies on strength reduction factors due to nonlinear behavior carried out in the last 30 years and put them in a common format in order to facilitate their direct comparison. A comparison of mean strength--reduction factors for systems subjected to ground motions recorded on firm alluvium sites from three different studies (Nassar and Krawinkler, 1991, Miranda, 1993; Riddell, 1995) is shown in Figure 1. The curve obtained by Nassar and Krawinkler was computed with 15 ground motions recorded in firm sites in California, Miranda's curve is computed from 62 ground motions recorded on firm alluvium sites in several countries during different earthquakes, while Riddell's curve is computed from 34 ground motions recorded on firm sites in Chile primarily during the march 3, 1985 earthquake. Although these studies are based on different sets of ground motions, the similarity of the results is remarkable and suggests that the general trends in reduction factors due to nonlinear behavior do not change significantly from one seismic region to another.
Based on the results of a comprehensive statistical study on strength-reduction factors of SDOF systems undergoing different levels of inelastic deformation when subjected to 124 ground motions, Miranda (1993) proposed simplified expressions to obtain analytical estimates of the strength-reduction factors for rock, alluvium and soft soil sites. Similarly, Nassar and Krawinkler (1991) and Riddell have recommended simplified expressions. However, none of these expressions have been incorporated into code provisions. Miranda's study showed that although some differences exist between strength reduction factors for rock and firm alluvium sites, for practical applications these differences are relatively small and can be neglected. If one makes such simplification and in the absence of more specific information on site conditions one could use the following simplified expression in the design of structures built on rock or firm sites:

where [mu] is the displacement ductility ratio and T is the period of vibration. Equation 2 is simpler than the equations previously proposed and as shown in Figure 2 has very good agreement with the statistical studies being only slightly more conservative.
For very soft soil sites, the shape of the [R subscript mu] spectrum is significantly different to that of rock and firm sites and strongly dependent on the predominant period of the ground motion [T subscript S]. Studies by Miranda have shown that the elastic and inelastic response of structures on very soft soil sites depends on the ratio of the fundamental period of the structure to the predominant period of the soft soil site, [T/T subscript S]. Similarly, strength-reduction factors for ground motions recorded on soft-soil sites exhibit strong variations with changes in the [T/T subscript S] ratio. For periods closer than the predominant period of the site (i.e., [T/T subscript S is approximately equal to 1)] [R subscript mu] is much larger than the target ductility. For systems with periods shorter than two thirds of the predominant period of the soil site, the strength-reduction factor is smaller than the target ductility, whereas for systems with periods longer than two times [T subscript S] the strength-reduction factor is approximately equal to the target ductility. Further discussion on the strength reduction due to nonlinear behavior in structures on soft soil sites as well as simplified expressions can be found in Miranda (1993, 1996).
The dispersion on strength-reduction factors have been recently studied (Miranda, 1993 1- Riddell, 1995). These studies have concluded that with the exception of very short periods (T < 0.2 s), the coefficient of variation (COV) of [R subscript mu] is approximately period independent and that the dispersion increases with increasing displacement ductility ratio. COV's vary from 0.2 for ductility ratios of 2 to 0.5 for ductility ratios of 6.
Nassar and Krawinkler (1991) and Miranda (1993) studied the influence of earthquake magnitude and epicentral distance on the strength-reduction factors. Both studies concluded that the effect of both parameters is negligible on [R subscript mu].

Miranda (1996) has shown that the use of approximate reduction Pictors like those computed with equation 2 combined with the use of smoothed linear elastic response spectra (SLERS) can lead to very good estimates inelastic strength demands (i.e., lateral strength required to control displacement ductility demands).

where [R subscript MDOF] is the ratio of the lateral yielding strength required in the MDOF structure to remain elastic to [F subscript yMDOF] which is the lateral yielding strength required in the MDOF structure to avoid story displacement ductility demands larger than the maximum tolerable story displacement ductility ratio [mu subscript i]; and [R subscript SDOF] is equal to the previously defined [R. subscript mu] factor.
A study of the [R subscript M] factor is currently being conducted by the author. As part of this study, three reinforced-concrete SMRSF 8, 12 and 16 stories high were designed according to a strong column-weak beam philosophy and were subjected to three ground motions with a variable amplitude until maximum story displacement ductilities of 3, 4 and 5 were produced and until the buildings remain totally elastic. Strength reduction factors for equivalent SDOF models of the buildings undergoing the same levels of displacement ductility demands when subjected to the same records were also computed. The equivalent SDOF systems had a period of vibration equal to the fundamental period of vibration of the MDOF structures. Table I shows the [R subscript M] factor computed for story displacement ductility ratios of 3, 4 and 5 when subjected to the three ground motions. Although these results are only preliminary, two general trends can be observed: (a) [R subscript M] decreases with increasing story displacement ductility ratio (design base shear in MDOF structures increases with respect to SDOF structures with increasing ductility ratio); (b) [R subscript M] decreases with increasing number of stories (design base shear in MDOF structures increases with respect to SDOF structures with increasing number of stories).
Based on these results and other limited results presented by Nassar and Krawinkler (1991), the following preliminary equation is proposed for [R subscript M]


where T and [mu] are the period of vibration and the maximum tolerable story displacement ductility demand in the NMOF structure, respectively. A comparison of available data with the results of Eq. 4 is shown in Figure 3. Caution should be exercised in the use of Eq. 4 for design purposes as it is based on only few results. Furthermore, it is intended only for regular buildings in plan and in elevation and designed with strong columns-weak beams, so the use of Eq. 4 for other situations can lead to unconservative results.

the design lateral strength. An additional strength reduction can be considered in the design of a structure to take into account the fact that structures usually have a lateral strength higher than the design strength. These additional reductions can be divided into reductions due to element overstrength [R subscript SE] which accounts for the increase the lateral strength of the structure from the design strength to the strength associated to the formation of the first plastic hinge and reductions due to redundancy, strain hardening and other factors [R subscript SS] which increase the lateral strength of the structure from the strength associated to the formation of the first plastic hinge to the strength associated to the formation of a mechanism. Thus the suggested reduction factor to be used in design would be given by:

For a more detailed discussion on strength reductions due to overstrength the reader is referred to Miranda (1991) or ATC (1995a).
The limits in story ductility demands, as well as the limits in interstory drift, vary with the structural system and with the performance level. For example, the maximum tolerable story ductility demand in a steel special-moment-resisting-space frame (SMRSF) is larger than for a concentrically-braced steel frame. Similarly, for the steel SMRSF the maximum tolerable demands will be different for example in the Life Safe performance level and for the Near Collapse performance level. Thus, during the preliminary design of a structure there is a need to estimate the lateral strength (lateral load capacity) of the structure that is required in order to limit the global (structure) displacement ductility demand and the global drift demand to a certain limit which results in the adequate control of local (i.e. story) ductility demands and interstory
drifts. If the elastic design spectra are known for each earthquake design level, the R factors permit an estimation of such required lateral strength, particularly for the life safe, near collapse and collapse performance levels. Implementation of R factors in performance-based design requires the specification of such maximum tolerable story ductility demands and maximum tolerable interstory drift demands for each structural system and for each performance level. An important contribution to presently proposed performance-based design methodologies would be the specification and calibration of such limits.
ATC,(1995a). Structural Response Modification Factors, ATC-19 Report, Applied Technology Council, Redwood City, California.
ATC, (1995b). A Critical Review of Current Approaches to Earthquake Resistant Design, ATC-34 Report, Applied Technology Council, Redwood City, California.
Bertero, V.V. (1986). "Evaluation of Response Reduction Factors Recommended by ATC and SEAOC," Proc. 3rd U.S. Natl Conf. on Earthquake Engrg, South Carolina, pp. 1663-1673.
Miranda, E. (1991). "Seismic Evaluation and Upgrading of Existing Buildings", PhD Thesis, University of California at Berkeley, May 1991.
Miranda, E. (1993). "Site-Dependent Strength Reduction Factors", Journal of Structural Engineering ASCE, Vol. 119, No. 12, 1993, pp, 3 505-3 519.
Miranda, E., and Bertero, V.V. (1994). "Evaluation of Strength Reduction Factors", Earthquake Spectra, Earthquake Engineering Research Institute, Vol. 10, No. 2, May 1994, pp 357-379.
Miranda, E., (1996). "Site-Dependent Seismic Demands for Nonlinear SDOF Systems," Paper 2128, Proc. Eleventh World Conf. on Earthquake Engrg., Acapulco, Mexico, June 1996.
Nassar, A. and Krawinkler, H. (1991). "Seismic Demands for SDOF Report No. 95, The John A. Blume Earthquake Engrg. Center, Stanford University.
NEHRP (1988), Recommended Provisions for the Seismic Regulations for New Buildings, Report 223 A, Federal Emergency Management Agency, Washington, D.C.
Riddell, R. (1995). "Inelastic Design Spectra Accounting for Soil Conditions," Earthquake Engrg. and Struct. Dynamics, Vol. 24, pp. 1491-1510.
SEAOC (1988). Recommended Lateral Force Requirements and Commentary, Structural Engineers Association of California, San Francisco, California.
Uang, C.-M. (1991). "Establishing R (or R subscript w) and [C subscript d] Factors for Building Seismic Provisions", Journal of Structural Engineering ASCE, Vol. 117, No. 1, 199 1, pp. 19-28.
Uniform Building Code (1988). International Conference of Building Officials, Whittier, California.