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Assessment of the Bill Emerson Memorial Bridge - FTP Directory ...

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Station D1 (before amplification) and <strong>the</strong>ir Fourier spectra are shown in Figures 6.4, 6.5and 6.6, respectively. From <strong>the</strong>se figures it can be inferred that <strong>the</strong> amplified peakacceleration is 0.57 g in transverse and longitudinal directions and 0.42 g in <strong>the</strong> verticaldirection. The Fourier spectra indicate that <strong>the</strong> rock motions have wide frequency rangeswith <strong>the</strong>ir dominant frequency at approximately 10 Hz. The amplified three-componentrock motions will be used as inputs to <strong>the</strong> FE model <strong>of</strong> <strong>the</strong> cable-stayed bridge to assess<strong>the</strong> structural conditions <strong>of</strong> main components in this section.Considering <strong>the</strong>ir critical role in maintaining <strong>the</strong> structural integrity <strong>of</strong> <strong>the</strong> bridge, twotowers and all cables are evaluated. Time history analysis was conducted to characterize<strong>the</strong> stress distribution on towers. To mimic <strong>the</strong> actual excitation condition, <strong>the</strong> 3-D FE <strong>of</strong><strong>the</strong> cable-stayed bridge was subjected to <strong>the</strong> amplified rock motions in three directionssimultaneously. Normally, <strong>the</strong> maximum moment will possibly occur at <strong>the</strong> bottoms <strong>of</strong><strong>the</strong> two towers, B and D, and at <strong>the</strong> intersections <strong>of</strong> tower columns and cap beams, A andC, as shown in Figure 6.11.At <strong>the</strong> lower part <strong>of</strong> Towers 2 and 3 up to <strong>the</strong> cap beams, <strong>the</strong> cross sections <strong>of</strong> all columnsare 3.66 m × 6.71 m (12 ft × 22 ft) in solid shape as shown in Figure 6.12(a). In <strong>the</strong> plane<strong>of</strong> each tower is a solid 2.44 m (8 ft)-wide RC wall, which will streng<strong>the</strong>n <strong>the</strong> in-planebehavior <strong>of</strong> <strong>the</strong> tower. Therefore, <strong>the</strong> out-<strong>of</strong>-plane behavior <strong>of</strong> <strong>the</strong> tower is expected to bemore critical at its bottom portion up to <strong>the</strong> cap beam. Above <strong>the</strong> cap beam, <strong>the</strong> crosssection <strong>of</strong> all columns is also in rectangular shape but with a hole in <strong>the</strong> center as shownin Figure 6.12(b). The hollow sections start at joints 374, 417, 432, and 475 in <strong>the</strong> FEmodel as shown in Figure 6.11,To determine <strong>the</strong> bending capacity <strong>of</strong> each section, moment curvature analysis wasperformed to evaluate <strong>the</strong> load-deformation behavior <strong>of</strong> a RC section, using <strong>the</strong> nonlinearstress-strain relationships <strong>of</strong> concrete and steel materials. In this study, <strong>the</strong> Whitney stressblock for concrete along with an elasto-plastic reinforcing steel behavior is used. Theflexural strength <strong>of</strong> each section was evaluated using <strong>the</strong> s<strong>of</strong>tware XTRACT developedby Imbsen & Associates, Inc (http://www.imbsen.com). In <strong>the</strong> analysis <strong>of</strong> <strong>the</strong> solidsection, <strong>the</strong> concrete wall was neglected since <strong>the</strong> 2.44 m (8 ft) RC concrete wallbasically behaves like an infilled wall. The dimension and reinforcement distribution inboth solid and hollow sections are based on <strong>the</strong> bridge drawings. The solid sections at Band D are reinforced with 356 No. 35 (#11) bars and <strong>the</strong> top hollow sections at A and C isreinforced with 464 No. 28 (#9) bars.85

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