SEISMIC ANALYSIS OF STEEL FRAMED BUILDINGS WITH SELF-CENTERING FRICTION DAMPING BRACES
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1 th International Conference on Earthquake Engineering Taipei, Taiwan October 12-13, 26 Paper No. 182 SEISMIC ANALYSIS OF STEEL FRAMED BUILDINGS WITH SELF-CENTERING FRICTION DAMPING BRACES Songye Zhu 1, Yunfeng Zhang 2, and Le-Wu Lu 3 ABSTRACT This paper deals with a novel type of passive energy dissipation device termed self-centering friction damping brace (SDB) and its application to seismic hazard mitigation of steel concentrically braced framed buildings. The SDB uses superelastic Nitinol wire strands to enable its self-centering mechanism and enhanced energy dissipation capacity is achieved by friction effect over the sliding surfaces of SDB. Unlike conventional passive damping devices, SDB has the potential to minimize the permanent drifts of concentrically braced frames after strong earthquakes and withstand several moderate earthquakes without the need for repair or replacement. Experimental results of SDBs presented here demonstrate its self-centering capability. Nonlinear time history analysis which involves a 3-story steel framed building subjected to two suites of twenty earthquake ground motions was conducted and the analysis results are presented in this paper. It is shown that SDB can effectively control the seismic response of framed building structures while minimizing their permanent drifts. Keywords: Braced frame, Damping, Friction, Seismic response, Self-centering, Shape memory alloy INTRODUCTION Conventionally designed structural systems dissipate energy by connection yielding or damages developed in structural components during earthquakes. Such a seismic design strategy may not be desirable for high seismic regions because of costly repairs required after strong or even moderate earthquakes. After the 199 Northridge earthquake, growing interests are given to a more logical seismic design approach which involves energy dissipation through supplemental damping system. Using this approach, the main structural system is designed to have little or no damage while the damping devices dissipate energy and can be replaced if damaged during an earthquake. Examples of such energy dissipation device are friction damper (Filiatrault and Cherry 1987), buckling-restrained brace (Uang et al. 2), metallic yield damper (Tsai and Tsai 1995) and many other types of dampers. Buckling-restrained braces (BRB), which have been developed to overcome the buckling problem of conventional braces in concentrically braced frames, are capable of yielding in both tension and compression (Sabelli et al. 23; Uang et al. 2). Buckling-restrained braced frames (BRBF) has been used extensively for seismic applications in Japan after the 1995 Kobe earthquake and is also 1 Graduate Research Assistant, ATLSS Research Center, Lehigh University, Bethlehem, PA, USA, soz2@lehigh.edu 2 Assistant Professor, ATLSS Research Center, Lehigh University, Bethlehem, PA, USA; yuz8@lehigh.edu 3 Professor Emeritus, ATLSS Research Center, Lehigh University, Bethlehem, PA, USA; lwl@lehigh.edu
2 gaining popularity in the United States after the 199 Northridge earthquake. BRBFs are desirable for seismic design and rehabilitation for their superior ductile performance. Nonlinear dynamic analysis by Sabelli et al. (23) has shown that the behavior of BRBFs is comparable and often better than that of conventional concentrically braced frames and moment frames. However, several potential problems such as tendency of BRBs to yield even under frequent earthquakes and large residual drifts after strong earthquakes have been identified by a few researchers (Sabelli 23; Kiggins and Uang 2). Costly repair after moderate earthquakes might be necessary due to these problems. Recently, an alternative seismic resisting system with self-centering capability has been attracting considerable interests (e.g., Kurama et al. 1999; Lu et al. 2; Ricles et al. 21; Christopoulos et al. 22). A flag-shaped hysteresis loop is typical of such self-centering systems. Self-centering systems have the ability to control damage and to reduce (or even eliminate) residual structural deformation, after strong earthquake events. It is worth noting that residual structural deformation is emphasized as a fundamental complementary parameter in the evaluation of structural (and non-structural) damage in the performance-based seismic design and assessment approach (Pampanin et al. 23). Friction damped braced (FDB) frames have been studied by Pall and Marsh (1982), Filiatrault and Cherry (1987), and Aiken et al. (1988). Their results show that properly designed FDB frame can outperform traditional moment frames and cross-braced moment resisting frames. The addition of friction dampers results in significant reduction in inter-story drifts and internal forces. Nims et al. (1993) developed a passive friction-based energy dissipation device termed Energy Dissipating Restraint (EDR), which has a self-centering capability. The EDR would be installed in a building as a part of the bracing system which resists seismically induced lateral forces. Special metals such as superelastic shape memory alloys (SMA) possess the self-centering hysteretic behavior. This paper presents a novel bracing element termed self-centering friction damping brace (SDB) which has a selfcentering capability and enhanced energy dissipation capacity through friction. A novel type of concentrically braced frame systems can be established with the use of SDB, which offers a potential solution to the potential problems associated with BRB frames. DEVICE MECHANICS AND TEST RESULTS The mechanical configuration of SDB is shown in Fig. 1. Like BRB, SDB would be typically installed in a concentrically braced frame building as part of the bracing system which resists lateral seismic loads. The SDB is comprised of two steel parts that can slide past each other. Superelastic Nitinol wire strands are attached to the two parts using special anchors. In order to increase the friction force over the sliding surface for enhanced energy dissipation, a pre-specified amount of normal force can be applied using the bolts, as shown in Fig. 1. Nitinol wire strands Bolts Anchor Figure 1. Schematics of the mechanical configuration of SDB Fig. 2-(a) shows the typical hysteretic behavior of superelastic Nitinol wire strands which contribute to the self-centering capability of SDB. This unique hysteresis is a result of stress-induced phase transformation from austenite to martensite and reverse transformation upon unloading (Grasser and Cozzarelli, 1992). This important characteristic is called superelasticity or pseudoelasticity, which involves certain energy dissipation with zero residual strain upon unloading. Fig. 2-(b) shows the friction force induced hysteresis. By properly adjusting the ratio between the yield strength of Nitinol wire strands and the friction forces, the final combined hysteresis loop exhibits a nearly selfcentering behavior, as shown in Fig. 2-(c).
3 F F F δ + δ = δ Nitinol wire strand Coulomb friction damping SDB w/ self-centering capability w/ good energy disssipating capability w/ enhanced energy dissipation & nearly self-centering capability (a) (b) (c) Figure 2. Illustration of the self-centering and energy dissipation mechanism of SDB Nitinol alloys have an inherent self-centering capability, high ductility and very long fatigue life compared to other SMA materials. For example, the maximum recoverable strain of superelastic Nitinol wires can reach up to 8%. The test conducted by the writers shows that Nitinol wires with a diameter of.58 mm can sustain over two thousands load cycles under 8% strains cycles. These superior properties of superelastic Nitinol wires form the physical basis on which SDBs can self-center and can be reused for several strong earthquakes without performance deterioration. The reusability of SDB is very appealing in the sense that it can enhance the robustness of structural system performance during strong aftershocks following a significant earthquake event, thus eliminating the need for unnecessary evacuation or inspection after strong earthquakes. Figure 3. External view of scaled SDB specimen in an MTS test machine To validate the concept of SDB, cyclic testing of scaled SDB specimens was conducted. Fig. 3 shows one the scaled SDB specimens under test, which has a length of 2.3 feet. Each wire strand was comprised of ten loops of superleastic Nitinol wires with a diameter of.58 mm. The length of the Nitinol wire strands was 25 mm (1 inch). The cyclic test was carried out at room temperature on an MTS servohydraulic test machine and the loading frequency is 2 Hz. Figs. -(a) to (c) show the measured hysteretic loops of the SDB specimens with different levels of friction force. The friction force was measured using the same loading protocol for the MTS test machine after removing the Nitinol wires. Figs. -(c) to (e) show the hysteresis of friction forces corresponding to Figs. -(a) to (c) respectively. For the tests corresponding to Figs. -(a) and -(d), no bolts were used to apply the normal force and lubricant oil was added to the sliding surfaces in SDB in order to minimize the friction force. As shown in Figs. -(a) and -(d), the friction force is negligible and this SDB specimen
4 has very limited energy dissipation capacity. With increasing level of friction force, the SDB specimens exhibit a hysteresis loop with enhanced energy dissipation capacity (see Figs. -(b) and - (c)). It is also seen in Figs. -(a) to (c) that the behavior of SDB is almost symmetrical under tension and compression, which is another advantage of SDB derived from its unique mechanical configuration in contrast to directly using SMA bars as bracing members in a concentrically braced frame structure. The unique configuration of SDB enables the direct transfer of applied load to the Nitinol wire strands in tension. Although SMA bars can undertake both tension and compression forces, a significant difference in the behavior of SMA bars under compression and tension stresses has been observed by Dolce et al. (2), which may cause problems in beam design due to unbalanced forces in chevronbraced configurations of frame structures. 12 (a) 12 (b) 12 (c) (d) (e) (f) Friction (kn) Friction (kn) Friction (kn) Figure. Test results of SDB specimens Prototype Building COMPARATIVE SEISMIC ANALYSIS OF SDB AND BRB FRAMES In this study, the 3-story frame structure (model 3vb2) developed by Sabelli et al. (21, 23) for a study on BRB frames is selected as the prototype structure for nonlinear dynamic analysis. This 3- story building is designed to be located in downtown Los Angeles with site class D (firm soil). The design of this building follows the FEMA building design criteria, in which a response of modification factor (R) of 8 is employed. Fig. 5-(a) shows the 3-story building plan and the locations of BRB frames. In this study, the SDBs will be placed in the same location of BRBs in this prototype building structure. The elevation of a typical BRB or SDB frame, as well as the section sizes of columns and beams is shown in Fig. 5-(b). The yield capacities of the BRBs in this frame were designed based on the computed equivalent static base shear (Sabelli 21). The tensile capacities of BRBs in the 1 st, 2 nd and 3 rd stories are 181 kn, 872 kn and 52 kn respectively, and the compression capacities were assumed to be 1.1 times their tension capacities, which is consistent with previous research results. The post-yield stiffness of BRBs is assumed to be 1% of its initial stiffness. In this study, the yield capacity of SDBs is set equal to the average of the tensile and compressive strength of corresponding BRBs. The lengths of superelastic Nitinol wire strands in SDBs is.7 m, which results in 8% strain in Nitinol wires at a 2% story drift ratio. In this study 8% strain is taken as the maximum recoverable strain, and if the strain in
5 Nitinol wires can be controlled below 8% during the earthquake, residual strain in Nitinol wires will be negligible and thus no repair or replacement of SDBs are necessary after the earthquake. The friction force between the two parts in SDB is set to be 38% of the yield capacity of the Nitinol wire strands in one side of SDB. With the goal of examining the benefits associated with friction damping, a self-centering brace without friction, denoted as SDB-NF, was also considered as a control case. It is noted that without friction damping, the SDB-NF needs to use more Nitinol wires than a regular SDB would require in order to obtain the same yield strength for the bracing element. 3' 3' 3' 3' 3' 3' 3' W1X8 BRB or SDB 3' 3' 3' 3' W12X96 W1X8 W1X8 W12X96 13' 13' 13' (a) Building plan (b) Braced frame elevation Figure 5. The prototype 3-story concentrically braced frame structure Nonlinear Time History Analysis Nonlinear time history analysis was carried out using the computer program DRAIN-2DX (Prakash et al. 1993). The time history analysis employs the suites of earthquake ground motions developed previously by Somerville et al. (1997) for use in the FEMA project on steel moment-resisting frames. In this study, the earthquake suites corresponding to downtown Los Angeles, California, were selected for seismic hazard levels corresponding to a 5% and 1% probability of exccedence in a 5 year period, each of which contains 2 records designated as LA1 - LA2 and LA1 - LA6, respectively. These twenty records were derived from fault-parallel and fault-normal orientations of ten earthquake records with adjustment in amplitude and frequency domain. It is worth noting that other researchers also used the same suites of earthquake ground motions in their previous research on BRB frames (e.g., Sabelli 23; Kiggins and Uang 2). In the nonlinear time history analysis, only one single braced bay was modeled and analyzed. Thus the seismic mass of each floor was calculated by dividing the total seismic floor masses by the number of braced bays in each principal direction (i.e., ¼ of the total dead load for the 3-story building). All beam-column connections except for those at the roof were modeled as being fixed by considering the effect of attached gusset plates while the ends of all braces were assumed as frictionless pins. Rigid floor diaphragm is assumed for this 3-story building and thus all nodes at the same floor are constrained together in the horizontal direction of the input ground motion. In order to approximately account for the stiffness contribution from all other columns in the unbraced frame, a column running the full height was added to the model. The moment of inertia of this column is equal to 133 in and its plastic modulus, Z = 29 in 3, which is the same as that in Sabelli (23). Global P- effect was also considered in the analysis. Element type 1 in DRAIN-2DX, i.e. the inelastic truss bar element, was used to simulate the hysteretic behavior of BRB. In order to simulate the hysteretic behaviors of SDBs, one new element in DRAIN- 2DX was developed in this study, which uses a modified Wilde model (Zhang and Zhu 26) to describe the superelastic behavior of Nitinol wire strands and consider the friction over the sliding surface of SDB. The parameters of the modified Wilde model are calibrated with the dynamic test data
6 from Nitinol wires of a.58 mm diameter. The loading frequency of the cyclic tension test is 2 Hz with a 6% strain amplitude, which is believed to be close to the seismic response of the prototype structure. Fig. 6 shows the typical hysteresis (i.e., the brace force vs. inter-story drift) of a single brace in the 3rd story of the prototype building frame for BRB, SDB and SDB-NF respectively. 8 (a) BRB 8 (b) SDB 8 (c) SDB NF Figure 6. Typical hysteretic behavior of single brace in 3rd story: (a) BRB; (b) SDB; (c) SDB-NF Results and Discussion Figs. 7 to 8 show the results of a comparative study of the seismic behaviors of BRB and SDB frames under the DBE suite of earthquake ground motions, i.e. with 1% of probability of exceedence in 5 years. Figs. 7-(a) and 7-(b) show the maximum drift ratios and residual drift ratios for the BRB and SDB frames subjected to the DBE suite of earthquake ground motions. SDB-NF represents the case in which SDB braces without friction were used. For the SDB-NF, energy is dissipated only through the hysteretic damping of Nitinol wires which give reduced energy dissipation compared with normal SDB. The mean values of the maximum drift ratios of BRB, SDB and SDB-NF frames are.77%,.86% and 1.9% respectively, while the mean residual drift ratios are.28% for the BRB frame and almost zero for both the SDB-NF and SDB frames. The large value for the maximum story drift associated with the SDB-NF frame can be explained by the fact that the stiffness and energy dissipation capacity of SDB-NF are smaller than those of corresponding BRB in this study. However, with the increase of energy dissipation and initial stiffness by utilizing the friction effect, SDB frames can achieve a control performance comparable to the BRB frame in terms of peak story drift. More interesting to note is that even with much greater peak drift ratios, SDB-NF frames still have far smaller residual drifts than the BRB frame. This significant reduction of residual drifts in both SDB- NF and SDB frames manifests the benefit due to the unique self-centering characteristic of this new bracing element. It is stated in FEMA-356 (2) that for steel moment frame the allowable transient and permanent drifts corresponding to the life safety performance level are 2.5% and 1.% respectively, and the allowable transient and permanent drifts corresponding to the immediate occupancy performance level are.7% and negligible respectively. For both the 3-story SDB and BRB frames, their transient story drifts were always less than 2.5% under all twenty ground motions in the DBE suite; furthermore, they were less than.7% under ten earthquake ground motions. The permanent story drifts of the 3-story SDB frames were negligible under all twenty ground motions, while large permanent story drifts were observed in BRB frame under 15 ground motions. Therefore the SDB frame is more likely to achieve a higher performance target than the BRB frame under design basis earthquakes. It is noted that with the Nitinol wire length specified in this study, the largest recoverable strain of 8% in Nitinol wires corresponds to a 2% story drift ratio in the 3-story prototype building structure. When transient story drift ratio exceeded 2% (as shown by the shaded area in Fig. 7-(a)), residual strain would occur in Nitinol wires and these wires would have to be replaced after earthquake. Since the peak story drift of the 3-story SDB frames were always less than 2% under twenty ground motions, the SDBs need not be replaced and thus the reusability of SDB is validated in a statistical sense. It is worth noting that
7 although SDB is capable of achieving much better performance than the SDB-NF, the SDB uses less amounts of Nitinol wires than the SDB-NF which is relative expensive material. Maximum Drift Ratio BRB SDB SDB NF Strain in Nitinol wires exceeds 8% LA2 LA LA6 LA8 LA1 LA12 LA1 LA16 LA18 LA2 Earthquake Ground Motion (a) Maximum drift ratios Residual Drift Ratio.1.5 BRB SDB SDB NF LA2 LA LA6 LA8 LA1 LA12 LA1 LA16 LA18 LA2 Earthquake Ground Motion (b) Residual drift ratios Figure 7. Maximum and residual drift ratios for 3-story buildings Drift Ratio.2.1 (a) 3rd Story BRB SDB Acceleration (m/s 2 ) (a) 3rd Story BRB SDB (b) 2nd Story 15 (b) 2nd Story Drift Ratio.1 Acceleration (m/s 2 ) (c) 1st Story 15 (c) 1st Story Drift Ratio.1 Acceleration (m/s 2 ) Figure 8. Inter-story drift time histories of the 3-story prototype building under LA Figure 9. Acceleration time histories of the 3- story prototype building under LA13
8 To better understand the seismic response behavior of the SDB frames, Figs. 8 and 9 present the time histories of the inter-story drifts and absolute acceleration respectively for the BRB and SDB frames subjected to the LA13 record from the DBE suite. The LA13 record was derived from the ground motion recorded at Newhall during the 199 Northridge earthquake. It is seen in Fig. 8 that the SDB frame has very small residual drifts in all three stories of the prototype building compared to those of the BRB frame. Fig. 9 shows the acceleration response of the SDB frame has the same magnitude as that of the BRB frame on all three floors. Fig. 1 shows the distribution of the ensemble average of the maximum and residual drift ratios along the height of the 3-story prototype building with either BRBs or SDBs. The ensemble average was calculated based on the twenty earthquake ground motion records in either the DBE suite or the frequent earthquake suite. Figs. 1-(a) and 1-(b) show the statistical results under the design basis earthquakes and frequent earthquakes (i.e. with 5% of probability of exceedence in 5 years) respectively. It is seen that the peak story drifts of the SDB frame were close to that of the BRB frame under both the design basis earthquakes and frequent earthquakes. The SDB frames have minimal residual story drifts under both design basis earthquakes and frequent earthquakes, while for the BRB frame, non-trivial residual story drifts occurred under both earthquake suites. The ensemble average of the residual drift ratios of the BRB frames are about 3% of the peak story drift ratio under both earthquake suites. Even under the frequent earthquakes, the peak strains of the BRBs exceeded its yield strain under fifteen ground motions out of a total of twenty records. This observation confirms the findings by other researchers (e.g., Uang et al. 2) that BRB tends to yield even under frequent earthquakes. (a) Residual Peak Residual Peak (b) 3 3 Floor level 2 Floor level Story drift ratio (%) Story drift ratio (%) Figure 1. Ensemble average of the peak and residual story drift ratios of the 3-story prototype building: (a) under design basis earthquakes with 1% probability of exceedence in 5 years; (b) under frequent earthquakes with 5% probability of exceedence in 5 years (legend: square = BRB frame, circle = SDB frame) CONCLUSIONS The seismic behavior of a novel concentrically braced structural frame system with self-centering capability is presented in this paper. An innovative type of bracing element termed self-centering friction damping brace (SDB) is proposed in this paper, which will be installed to concentrically braced frame buildings as part of the bracing system. The SDBs thus resist the lateral seismic loads in such concentrically braced frame buildings. The mechanical configuration of SDB is described in this paper. In SDB, superelastic Nitinol wire strands are used as core component to provide the selfcentering capability while friction damping is utilized for enhanced energy dissipation. By adjusting the ratio between the yield strength of superelastic Nitinol wires and friction force in SDB, hysteresis loops with nearly self-centering behavior can be obtained for SDB. A proof-of-concept test on scaled SDB specimens was carried out in this study and experimental results validate the anticipated hysteretic behavior of SDB. Due to the unique behavior of superelastic Nitinol wires, SDB can be designed to withstand several design basis earthquakes without the need for replacement or repair.
9 A comparative study of the seismic responses of 3-story nonlinear frames with buckling-restrained braces (BRBs) and SDBs was carried out by using the computer program DRAIN-2DX. Two suites of earthquake ground motions each containing 2 earthquake records were used for frequent and design basis earthquakes respectively. The nonlinear time history analysis result shows that compared with BRB frames, SDB frames have significantly reduced residual story drifts while still capable of achieving a control effect comparable to the BRBs in terms of peak story drifts and acceleration responses. The analysis results also demonstrate the enhanced performance of SDB owing to its friction damping. This study also confirms the findings by other researchers that BRB tends to yield even under frequent earthquakes, which might require costly repair. SDB has the potential to realize damage free structural frame systems under frequent and design basis earthquakes. ACKNOWLEDGEMENTS Travel grant received from NSF to attend the US-Taiwan Workshop on Smart Structural Technology for Seismic Hazard Mitigation is gratefully appreciated. The authors are also grateful to the Pennsylvania Infrastructure Technology Alliance and Lehigh University for providing additional financial support for this research. However, the findings, opinions and conclusions expressed in this paper are solely those of the writers and do not necessarily reflect the views of the sponsors. REFERENCES Aiken, I.D., Kelly, J.M. and Pall, A.S. (1988) Seismic response of a nine-story steel frame with friction damped cross-bracing, Report No. UCB/EERC-88/17, University of California, Berkeley, CA. Christopoulos, C., Filiatrault, A., and Folz, B. (22) Seismic response of self-centering hysteretic SDOF systems, Earthquake Engineering and Structural Dynamics, 31, Filiatrault, A. and Cherry, S. (1987) Performance evaluation of friction damped braced frames under simulated earthquake loads, Earthquake Spectra, 3(1), Kiggins, S. and Uang, C.M. (2) Reducing residual drifts in BRBF systems, Proc. of 73 rd SEAOC Annual Convention, Sacramento, CA, Kurama, Y., Sause, R., Pessiki, S. and Lu, L.-W. (1999) Lateral load behavior and seismic design of unbonded post-tensioned precast concrete walls, ACI Structural Journal, 96(), Lu, L.-W., Sause, R., Ricles, J.M., and Pessiki, S.P. (21). High Performance, Cost Effective Structural Systems for Seismic-Resistant Buildings. Earthquake Engineering Frontiers in the New Millennium, Proceedings, U.S.-China Millennium Symposium on Earthquake Engineering, pp Nims, D.K., Ritcher, P.J., and Bachman, R.E. (1993). The use of the energy dissipating restraint for seismic hazard mitigation, Earthquake Spectra, 9(3): Pall, A.S. and Marsh, C. (1982) Response of friction damped braced frames, J. Struct. Div., ASCE, 18(ST6), Pampanin, S., Christopoulos, C. and Priestley M.J.N. (23) Performance-based seismic response of frame structures including residual deformations, Part II: multidegree-of-freedom systems, Journal of Earthquake Engineering, 7(1): Prakash, V., Powell, G.H., and Campbell, S. (1993). DRAIN-2DX: Base Program and User Guide, Report No. UCB/SES-93/17, University of California, Berkeley, CA. Ricles, J.M., Sause, R., Garlock, M.M., and Zhao, C. (21) Post-tensioned seismic-resistant connections for steel frames, Journal of Structural Engineering, 127(2): Sabelli, R. (21) Research on improving the design and analysis of earthquake-resistant steel-braced frames, The 2 NEHRP Professional Fellowship Report, EERI, Oakland, CA. Sabelli, R., Mahin, S.A., and Chang, C., (23) Seismic demands on steel-braced buildings with bucklingrestrained braces, Engineering Structures, 25,
10 Sommerville, P., et al. (1997) Development of ground motion time histories for Phase 2 of the FEAM/SAC steel project, SAC Background document SAC/BD-91/, SAC joint venture, Sacramento, California. Tsai, C.S., and Tsai, K.C. (1995) TPEA device as seismic damper for high-rise buildings, ASCE Journal of Engineering Mechanics, 121(1): Uang, C.M., Nakashima, M., and Tsai, K.C., (2) Research and application of buckling-restrained braced frames, International Journal of Steel Structures,, Wilde, K., Gardoni, P., and Fujino, Y. (2). Base isolation system with shape memory alloy device for elevated highway bridges, Eng. Struct., 22(3), Zhang, Y. and Zhu, S. (26) Seismic response control of building structures with superelastic shape memory alloy wire Damper, ASCE Journal of Engineering Mechanics, in review.
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