110-dynamic behavior and seismic retrofitting method for half-through steel arch bridges subjecte

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 1 INTRODUCTION When a strong earthquake occurs, steel arch bridges and steel bridge piers are frequently subjected to fault displacement induced by ground motion (Japan Society of Civil Engineering 1999a,b). Thus, it is still necessary to establish a method concerning the effect of fault displacement to check the seismic performance developed from nonlinear dynamic analysis for arch bridge design. Furthermore, it is needful to construct steel arch bridges possessing high seismic capacity at a minimum cost. Half-through type steel arch bridge is one of the arch  bridges which reveal complicated behavior when subjected to ground motion or fault displacement and ground motion. However, seismic performance and failure behavior have not  been y et c larified and only few studies concerning nonlinear seismic analysis when subjected to fault displacement have been reported (Yamao et al. 2007). This paper presents the results of nonlinear dynamic response analysis of a half-through type steel arch bridge subjected to fault displacement including earthquake waves in transverse and longitudinal (expanding and shrinking) directions. In this study, the fault displacement induced  by the ground motion was assumed to occur at the surface of the earth in the middle of the  bridge span as shown in Fig.1. In dynamic response analyses, the loading conditions were adjusted by controlling two different fault displacement waves at both ends of stiffened girders and at both springings of arch ribs. That is, both the fault displacement wave obtained from the time integral of the acceleration response wave and the ground motion simulated from the 1999 Taiwan Ji-Ji Earthquake wave were input. The seismic behavior of the bridge model subjected to the fault displacement including ground motion was investigated. Finally, in order to control the seismic demand of a half-through steel arch bridge, the seismic retrofitting methods were  proposed and we discussed the effect of the proposed method s on the seismic behavior of the  bridge model. Dynamic behavior and seismic retrofitting method for half-through steel arch bridges subjected to fault displacement Toshitaka Yamao  Dept. of Civil and Environmental Engineering, Kumam oto University, Kumamoto, Japan Yoshie Tsujino Obayashi Corporation Co. Ltd. Institution, Tokyo, Japan Zhanfei Wang Civil Engineering College, Shenyang Jianzhu University, Shenyang, China ABSTRACT: This paper presents the seismic behavior of dynamic response analyses and seismic retrofitting of half-through steel arch bridges subjected to fault displacement. Both the 1999 Taiwan Ji-Ji Earthquake wave and the fault displacement wave obtained from the time integral of the acceleration response wave were applied and the response behavior was investigated. The dynamic response analyses were carried out using earthquake waves including fault displacement in transverse and longitudinal (expanding and shrinking) directions in order to investigate seismic behavior of bridge models. According to the analytical results, it was found that the plastic members were clustered near the intersections of arch ribs and stiffened girders and at the union of stiffened girders and end support. Finally, the effect of the proposed seismic retrofitting methods on the seismic behavior of the bridge model was discussed.

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8/12/2019 110-Dynamic Behavior and Seismic Retrofitting Method for Half-through Steel Arch Bridges Subjecte

http://slidepdf.com/reader/full/110-dynamic-behavior-and-seismic-retrofitting-method-for-half-through-steel 1/9

 

1 INTRODUCTION

When a strong earthquake occurs, steel arch bridges and steel bridge piers are frequentlysubjected to fault displacement induced by ground motion (Japan Society of Civil Engineering1999a,b). Thus, it is still necessary to establish a method concerning the effect of faultdisplacement to check the seismic performance developed from nonlinear dynamic analysis forarch bridge design. Furthermore, it is needful to construct steel arch bridges possessing highseismic capacity at a minimum cost. Half-through type steel arch bridge is one of the arch

 bridges which reveal complicated behavior when subjected to ground motion or faultdisplacement and ground motion. However, seismic performance and failure behavior have not

 been yet clarified and only few studies concerning nonlinear seismic analysis when subjectedto fault displacement have been reported (Yamao et al. 2007).

This paper presents the results of nonlinear dynamic response analysis of a half-through typesteel arch bridge subjected to fault displacement including earthquake waves in transverse andlongitudinal (expanding and shrinking) directions. In this study, the fault displacement induced

 by the ground motion was assumed to occur at the surface of the earth in the middle of the bridge span as shown in Fig.1. In dynamic response analyses, the loading conditions wereadjusted by controlling two different fault displacement waves at both ends of stiffened girdersand at both springings of arch ribs. That is, both the fault displacement wave obtained from thetime integral of the acceleration response wave and the ground motion simulated from the 1999Taiwan Ji-Ji Earthquake wave were input. The seismic behavior of the bridge model subjectedto the fault displacement including ground motion was investigated. Finally, in order to controlthe seismic demand of a half-through steel arch bridge, the seismic retrofitting methods were

 proposed and we discussed the effect of the proposed method s on the seismic behavior of the bridge model.

Dynamic behavior and seismic retrofitting method forhalf-through steel arch bridges subjected to fault displacement

Toshitaka Yamao Dept. of Civil and Environmental Engineering, Kumamoto University, Kumamoto, Japan

Yoshie TsujinoObayashi Corporation Co. Ltd. Institution, Tokyo, Japan

Zhanfei WangCivil Engineering College, Shenyang Jianzhu University, Shenyang, China

ABSTRACT: This paper presents the seismic behavior of dynamic response analyses andseismic retrofitting of half-through steel arch bridges subjected to fault displacement. Both the1999 Taiwan Ji-Ji Earthquake wave and the fault displacement wave obtained from the timeintegral of the acceleration response wave were applied and the response behavior wasinvestigated. The dynamic response analyses were carried out using earthquake waves includingfault displacement in transverse and longitudinal (expanding and shrinking) directions in orderto investigate seismic behavior of bridge models. According to the analytical results, it wasfound that the plastic members were clustered near the intersections of arch ribs and stiffenedgirders and at the union of stiffened girders and end support. Finally, the effect of the proposedseismic retrofitting methods on the seismic behavior of the bridge model was discussed.

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Toshitaka Yamao, Yoshie Tsujino and Zhanfei Wang 867

13900

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10600

2  2   0  

 0  

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Figure 1 : Half-through arch bridge (unit: mm)

2 SEISMIC RESPONSE ANALYSIS

2.1 Theoretical arch model

The theoretical arch model studied herein is representative for actual half-through type arch bridges as shown in Fig.1.The theoretical model, in which 11 vertical columns are hinged to

arch ribs at both ends. The arch has a span length ( l ) of 106 m and the arch rise ( f ) is 22 m. Theglobal axis of the arch ribs are also shown in Fig.2(a),(b), where b and L represent the width of astiffened girder and the deck span, respectively. The cross sectional profiles of vertical membersand lateral members are rectangular and I-sections as shown in Figure 3(b) and 3(c). The modelwas assumed to have no residual stresses and initial crookedness modes. Material properties ofthe models used in the numerical analyses were assumed to be SM490Y steel type (JIS) with theyield stress (σy) of 353 MPa  and Young’s modulus E was 206 GPa, respectively. Archrise-to-span ratio ( f/l ) was taken to be 0.21 according to the condition of the actual arch bridges.

f=22.0m

l  =106.0

71.0

f=22.0m

l  =106.0

71.0

l  =106.0

71.0

 

 b=12.3

L=139.0

 b=12.3

L=139.0  

(a) (b)

914

1516

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14

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 (c) (d) (e)

Figure 2 : Theoretical arch model (unit: m):(a)Global view of theoretical model, (b)Plane view oftheoretical model, (c)Arch rib, (d)Vertical column, (e)Lateral member

2.2 Input seismic waves

The fault displacement wave used in this analysis was obtained from the time integral of theacceleration response wave, that is, the ground motion simulated from the 1999 Taiwan Ji-JiEarthquake wave as shown in Fig.5. For the 1999 Taiwan Ji-Ji Earthquake input wave, the

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868 ARCH’10 – 6th International Conference on Arch Bridges

relative large fault displacement measured after the earthquake was also concerned. Fig.6(a)illustrates three fault displacement waves TCU68EW2-3, TCU68EW2-5 and TCU68EW2-6and the residual displacements of these waves are different. Fig.6(b) shows the relativedisplacement curve for different two fault displacement waves and the maximum relative faultdisplacement is 3m. In the dynamic response analyses, both the seismic waves and the faultdisplacement wave were input in order to simulate the movement at both ends of stiffened

girders and at both arch springing. In relative fault displacements 1m, the TCU68EW2-5 wavewas applied at the left arch sprnging and the TCU68EW2-6 wave was applied at the right archsprnging in longitudinal or transverse directions, as mentioned in Fig. 4, respectively. Therelative fault displacement is changed 1-3m by combination of two fault displacement wavesas shown in Fig.6(b).

Figure 4 : Loading conditions in seismic faultdisplacement analysis

Figure 5 : 1999 Ji-Ji Earthquake wave 

20 30 40 50 60 70 800

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EW5&6(96.2cm)

EW3&5(201.9cm)EW3&6(298.1cm)

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(a) (b)

Figure 6 : Input fault displacement wave:(a)Input fault displacement wave, (b)Relative displacement

2.3 Eigenvalue analysis

The eigenvalue analysis was carried out to investigate the effect of arch ribs and stiffenedgirders on the natural periods of the bridge model. In order to understand the fundamentaldynamic characteristics, Table 1 presents the natural periods and the effective mass ratios ofeach predominant mode. The maximum effective mass ratios obtained in X, Y and Z directionsimply the order of the dominant natural period. It can be seen from Table 1 that the arch bridgemodel is possible to vibrate sympathetically at the 1st mode in longitudinal direction (X-axis),2th and 5th modes in transverse direction (Y-axis) and 8th mode in-plane direction (Z-axis),respectively.

0 20 40 60 80

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Fault

Transversedirection

Longitudinaldirection

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[cm]

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TCU068EW2-3TCU068EW2-5TCU068EW2-6

    絶    対    変    位

Time (sec)   A   b  s  o   l  u   t  e   f  a  u   l   t   d   i  s  p   l  a  c  e  m  e

  n   t

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Table 1 : Result of eigenvalue analysis

Order of period Natural frequency(Hz) Natural periods(sec) Effective massratio (%)

X Y Z

1 1.1038 0.90593 39 0 0

2 1.8226 0.54866 0 37 0

3 3.2313 0.30948 0 0 0

4 3.5552 0.28128 11 0 0

5 3.7638 0.26569 0 40 0

6 4.1324 0.24199 0 5 0

7 4.3546 0.22964 0 0 0

8 4.594 0.21767 0 0 40

9 5.1533 0.19405 0 0 15

10 5.6619 0.17662 0 1 0

2.4 Damping matrix and numerical analysis

 Numerical analyses were conducted using the Newmark-β  method (β  = 0.25) where theequations of motion were integrated with respect to time taking into account geometricalnon-linearity. A constant time step of 0.001 sec and a damping model (Rayleigh type) calibratedto the initial stiffness and mass were utilized. The seismic response analysis with groundacceleration input and a constant dead load was performed using the nonlinear FEM programTDAPIII (NIPPON TDAPIII 2005), which is capable of taking into account materialnon-linearity.

3 RESPONSE BEHAVIOR OF FALUT DISPLACEMEENT

3.1 Distribution of plastic zones

Fig.7 illustrates the deformation modes of the arch bridge in longitudinal direction (expandingand shrinking) when 3.0 m relative displacement was applied. The yielded memberscorresponding to the deformation mode subjected to 1.0 m relative displacement are alsoillustrated in Fig.8. It can be seen that the plastic members are clustered beneath the joints of thearch ribs, end vertical columns and stiffened girders. This is caused by the large deformation atthis intersection zones as shown in Fig.7. Fig.9 shows some element numbers of the theoreticalmodel in order to illustrate the plastic ratios of strain for these members.

(a) (b)

Figure 7 : Deformation modes of theoretical modeltic analysision dgeion. Direction:(a)Longitudinaldirectiong(Shrinking), (b)Longitudinal direction(Expanding)

3.2 Distribution of maximum and minimum plastic ratios of strain

Fig.10 shows the distribution of the maximum and the minimum plastic ratios of strain responseof the arch rib and the stiffened girder in longitudinal direction. The strain ratio was plotted at1.0m, 2.0m and 3.0m of relative displacement applied and non-dimensionalized parameter. The

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870 ARCH’10 – 6th International Conference on Arch Bridges

results coincide with the locations of yielded elements where the maximum strains of the archrib occurred beneath the joints of the arch rib and the stiffened girder.

(a) (b)

Figure 8 : Distributions of tic analysision dgeion.direction:(a) Longitudinal directiong(Shrinking),(b)Longitudinal direction(Expanding)

(a) (b)

Figure 9 : Main element numbers of theoretical modeltic analysision dgeion direction(a)Arch rib andvertical columns, (b)Stiffened

(a)

(b)

Figure 10 : Distribution of maximum and minimum plastic ratios of strain response in longitudinaldirection : (a) Longitudinal direction (shrinking), (b) Longitudinal direction (expanding)

The distribution of the maximum and the minimum plastic ratios of strain response of the archrib, the stiffened girder and vertical column in transverse direction were illustrated in Fig.11.From these figures, it was found that maximum and minimum strain ratios in transversedirection were relatively small and were nearly equal to 1.2. The results coincide also with the

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要素番号

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     y

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locations of yielded elements where the maximum strains of the arch rib occurred beneath the joints of the arch rib and the stiffened girder.

(a) (b)

(c)

Figure 11 : Distributions of maximum and minimum plastic ratios of strain response in transverse

direction:(a)Arch rib, (b)Stiffened girder, (c)Vertical column

Figure 12 : Stress-strain relation of BRB Figure 13 : Installed positions of BRB

Table 2 : Cross section area of BRB

Yield stress Cross section area Yield force[MPa] [cm

2] [kN] 

Original model 235 203.700 5,900

BRB 235 60.000 1,410 

4 SEISMIC RETROFITTING METHOD OF HALF-THROUGH ARCH BRIDGE

4.1 Outline of seismic retrofitting method

From analytical results, it was recognized that this bridge needs to control the seismic demandsince the structural damage by the fault displacement is so large. Then we tried to improve theseismic response using two retrofitting methods, that is, the installation of buckling-restrained

 brace (BRB) and the modified box and I-section with the increment bending stiffness at the

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intersections of the arch rib and the stiffened girder. BRBs are used recently as a structuralcontrol device in bridge structures. BRBs in this paper were assumed to have a stress-strain

 property, Young’s modulus E=213GPa and E’/60 as shown in Fig.12 and Table 2 shows thecross section area of BRB. BRBs are installed at the locations of bold line in Fig.13 instead ofdamaged members. In order to increase the bending stiffness about Y-axis rotation, thethickness of web plates for arch ribs and stiffened girder was changed from 1.2 cm to 5.6 cm.

4.2 Distribution of plastic zones of seismic retrofitting model

Fig.14 illustrates the yielded members (red line members) of the seismic retrofitting modelswith BRBs and incremental stiffness in transverse direction when 3.0 m relative displacementwas applied. Though the yielded members of the seismic retrofitting model were able to reducein comparison with results of the original model, there are some yielded members at theintersections of the arch rib and the stiffened girder, and it is not sufficient for the seismicdemand which all members are elastic. It is necessary to propose the more suitable seismicretrofitting method for the fault displacement.

(a) (b)

Figure 14 : Yield members in transverse direction (3m) : (a)BRB model, (b) Incremental stiffness model

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(b)

Figure 15 : Distributions of maximum and minimum plastic ratios of strain responsein longitudinal

direction : (a) Arch rib, (b)Stiffened girder

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1000 1020 1040 1060 1080 1100-2

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(a) (b)

Figure 16 : Distributions of maximum and minimum plastic ratios of strain response in transversedirection

4.3 Distribution of maximum and minimum plastic ratios of strain 

Fig.15 shows the distribution of the maximum and the minimum plastic ratios of strain responseof the arch rib and the stiffened girder in longitudinal direction. From these figures, it can berecognized that the effect of the seismic retrofitting method with the incremental stiffness on themaximum and minimum strain response of the arch ribs in longitudinal direction was large andits value ε/εy was equal to or less than 1.0. However, the effects of the seismic retrofittingmethod with BRBs were not able to be seen. This caused by the relatively small ground motionand the dominant seismic behavior of the fault displacement. Fig.16 illustrates the distributionof the maximum and the minimum plastic ratios of strain response of the arch rib and thestiffened girder in transverse directions. It was found that the maximum and the minimum

 plastic ratios (ε/εy ) of strain response of the arch rib and the stiffened girder were not more than

1.0 by the seismic retrofitting method with the incremental stiffness.

5 CONCLUSIONS

Seismic behavior of the half-through steel arch bridge subjected to fault displacement includingground motions in transverse and longitudinal directions were investigated by dynamic responseanalyses. In dynamic response analyses, the loading conditions were adjusted by controlling twodifferent fault displacement waves at both ends of stiffened girders and at both springings ofarch ribs. The seismic behavior of the bridge model subjected to the fault displacementincluding ground motion was investigated. Finally, in order to control the seismic demand of ahalf-through steel arch bridge, the seismic retrofitting methods were proposed and we discussedthe effect of the proposed methods on the seismic behavior of the bridge model. Theconclusions of this study are summarized as the followings. 

(1) The effect of the fault displacement wave direction on the damage of the half-throughsteel arch bridge model is dominant;

(2) The results obtained from dynamic response analyses indicate that the plastic membersare clustered near the joints of the arch ribs and stiffened girders. This is caused by the largedeformation at this intersection zones;

(3) The effect of the seismic retrofitting method with the incremental stiffness on themaximum and minimum strain response of the arch ribs in longitudinal or transverse directionswas large and its value ε/εy was equal to or less than 1.0;

(4) The effects of the seismic retrofitting method with BRBs on the controlling the seismicdemand of the half-through steel arch bridge subjected to fault displacement including groundmotions were not able to be seen.

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REFERENCES

Japan Society of Civil Engineering. 1999a. The 1999 Ji-Ji Earthquake,Taiwan-Investigation into

Damage to Civil Engineering Structure. 

Japan Society of Civil Engineering. 1999b. The 1999 Kocaeli Earthquake,Turkey-Investigation into

Damage to Civil Engineering Structure. 

Japan Road Association. 2002. Specifications for Highway Bridges, Part ΙΙ  Steel Bridge and Part VSeismic Design. (in Japanese)

 NIPPON TDAPIII. 2005. Ver2.13 User Manual.

Yamao, T., Takaji T. and Atavit S. 2006. Ultimate strength and behavior of deck-type arch bridges with

curved pair ribs, Proc. of Fourth International Conference on New Dimensions in Bridges, Flyovers &

Elevated Structures, Fuzhou, China, p.317-324.

Yamao, T., Sho T., Murakami S. and Mazda T. 2007. Seismic behavior and evaluation of seismic

 performance of half through steel arch bridges subjected to fault displacement, Journal of Seismic

Engineering , p.317-324.