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The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong><br />

Wind Engineering, November 8-12, 2009,<br />

Taipei, Taiwan<br />

WIND TUNNEL STUDY ON AERODYNAMIC OPTIMIZATION OF<br />

SUSPENSION BRIDGE DECK BASED ON FLUTTER STABILITY<br />

Qi Wang 1 Hai-li Liao 2 and Ming-shui Li 3 R<strong>on</strong>g Xian 4<br />

1 PhD Student, Research Centre for Wind Engineering, Southwest Jiaot<strong>on</strong>g University<br />

Chengdu Sichuan 610031, PR China, wangchee_<str<strong>on</strong>g>wind</str<strong>on</strong>g>@swjtu.edu.cn<br />

2 Pr<strong>of</strong>essor, Civil engineering school, Southwest Jiaot<strong>on</strong>g University<br />

Chengdu Sichuan 610031, PR China, hlliao@swjtu.edu.cn<br />

3 Pr<strong>of</strong>essor, Research Centre for Wind Engineering, Southwest Jiaot<strong>on</strong>g University<br />

Chengdu Sichuan 610031, PR China, lms_rcwe@126.com<br />

4 PhD Student, Research Centre for Wind Engineering, Southwest Jiaot<strong>on</strong>g University<br />

Chengdu Sichuan 610031, PR China, rxianok@163.com<br />

ABSTRACT<br />

Nanjing the 4th bridge <strong>of</strong> Yangtze River is a three span suspensi<strong>on</strong> bridge <strong>of</strong> main span lengths 1418m, and the<br />

flutter checking <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is up to 60.8m/s for the completed bridge. Through a 1:50 scale secti<strong>on</strong> model, more<br />

than 40 model cases were tested in order to obtain an optimized <strong>aerodynamic</strong> c<strong>on</strong>figurati<strong>on</strong> <strong>of</strong> the girder. The<br />

influence <strong>of</strong> modificati<strong>on</strong>s <strong>of</strong> the accessory comp<strong>on</strong>ents and the geometry <strong>on</strong> the <strong>aerodynamic</strong> stability has been<br />

established through this <str<strong>on</strong>g>study</str<strong>on</strong>g>, which has been beneficial to the final design <strong>of</strong> the bridge. At last, this paper tries<br />

to discuss the mechanism <strong>of</strong> the flutter <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed increasing.<br />

KEYWORDS: NANJING 4 TH BRIDGE OF YANGTZE RIVER, TRAPEZOIDAL BOX SECTION,<br />

AERODYNAMIC CONFIGURATION, OPTIMIZATION, WIND TUNNE TEST,<br />

Introducti<strong>on</strong><br />

Nanjing 4th bridge <strong>of</strong> Yangtze river in Jiangsu Province <strong>of</strong> southeast <strong>of</strong> China is a<br />

three span suspensi<strong>on</strong> bridge with main span 1418m. The original design <strong>of</strong> bridge deck is a<br />

trapezoidal steel box girder with overall width <strong>of</strong> 37.7m and a height <strong>of</strong> 3.4m, see Fig.1.<br />

According to the <str<strong>on</strong>g>wind</str<strong>on</strong>g> statistic data and the Chinese Code <strong>of</strong> Bridge Wind Resistance,<br />

the flutter checking <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed <strong>of</strong> the bridge is up to 60.8m/s, the <strong>aerodynamic</strong> stability<br />

becomes a governing factor in the design. Unfortunately the flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed <strong>of</strong> the<br />

original girder is less than 45m/s, which was found by intensive <str<strong>on</strong>g>wind</str<strong>on</strong>g> <str<strong>on</strong>g>tunnel</str<strong>on</strong>g> testing <strong>of</strong> secti<strong>on</strong><br />

model. Because <strong>of</strong> its intrinsic limit in the aspect <strong>of</strong> flutter instability, it is necessary to adopt<br />

some countermeasures to improve <strong>aerodynamic</strong> performance to meet the requirements <strong>of</strong><br />

<str<strong>on</strong>g>wind</str<strong>on</strong>g> resistance code. Aerodynamic optimizati<strong>on</strong> <strong>of</strong> the deck c<strong>on</strong>figurati<strong>on</strong> is hence definitely<br />

required to ensure the safety <strong>of</strong> the bridge.<br />

Through a 1:50 scale secti<strong>on</strong> model, more than 40 c<strong>on</strong>figurati<strong>on</strong> cases <strong>of</strong> deck were<br />

tested in order to establish the influence <strong>of</strong> the accessory comp<strong>on</strong>ents and the geometrical<br />

modificati<strong>on</strong>s <strong>on</strong> the <strong>aerodynamic</strong> stability, such as the porosity <strong>of</strong> railing in the sideway, the<br />

positi<strong>on</strong> <strong>of</strong> inspecti<strong>on</strong> rail, the guide wing, the edge c<strong>on</strong>figurati<strong>on</strong> <strong>of</strong> the secti<strong>on</strong>, the steepness<br />

<strong>of</strong> side wall slopes. Those countermeasures have been proved to be effective to improve the<br />

<strong>aerodynamic</strong> performance particular flutter instability <strong>of</strong> bridge by other researchers and<br />

engineering practices (A. Larsen, 1993; K. Wilde et al., 2001; B. Luca et al., 2002; S<strong>on</strong>g<br />

Jinzh<strong>on</strong>g et al., 2002; T. Miyata, 2003; Liu Cijun et al., 2008; Y<strong>on</strong>gxin Yang et al., 2008 ). In<br />

The work described in this paper was supported by the grants from the Nati<strong>on</strong>al Natural Science Foundati<strong>on</strong> <strong>of</strong> China<br />

(Project No. 90815016)


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

this paper their sensitivity relative to <strong>aerodynamic</strong> stability were investigated through a series<br />

<strong>of</strong> secti<strong>on</strong> model <str<strong>on</strong>g>wind</str<strong>on</strong>g> <str<strong>on</strong>g>tunnel</str<strong>on</strong>g> testing. The results has benefited for the final design <strong>of</strong> the<br />

bridge, and other l<strong>on</strong>g span bridges.<br />

Figure 1: Outline <strong>of</strong> Nanjing Yangtze 4th Bridge<br />

The Influence <strong>of</strong> Railing <strong>on</strong> Flutter Critical Wind Speed<br />

In order to examine the influence <strong>of</strong> the different railing and its positi<strong>on</strong> <strong>on</strong> the critical<br />

<str<strong>on</strong>g>wind</str<strong>on</strong>g> speed, two kinds <strong>of</strong> railing with porosity 90% and 60%, three locati<strong>on</strong>s <strong>of</strong> railing <strong>on</strong><br />

deck, <strong>on</strong>e is <strong>on</strong> the edge (the original design), the others are 5mm (prototype 250mm) and<br />

10mm (prototype 500mm) from the sideway edge, are chosen to be tested. The results are<br />

given in table 1. It is found that higher <strong>aerodynamic</strong> stability for the railing with higher<br />

porosity comparing to the lower <strong>on</strong>e. This similar finding was also reported by Allan Larsen<br />

in the <strong>aerodynamic</strong> design <strong>of</strong> Great belt East Bridge (A. Larsen, 1993), and other researchers<br />

(B. Luca et al., 2002; T. Miyata, 2003; Liu Cijun et al., 2008). Comparing to the secti<strong>on</strong><br />

c<strong>on</strong>figurati<strong>on</strong> <strong>of</strong> old Tacoma Bridge deck, see fig.2, the low porosity <strong>of</strong> railing has made the<br />

deck c<strong>on</strong>figurati<strong>on</strong> close to I-shape, which may lead to flow separati<strong>on</strong>, and a vortex shedding<br />

in a rhythmic fashi<strong>on</strong> will generate separati<strong>on</strong> bubbles above the deck (see fig3). The vortex<br />

creati<strong>on</strong> and drift process will dramatic weaken the stability <strong>of</strong> the girder. However, the<br />

critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed <strong>of</strong> girder is not sensitive to the change <strong>of</strong> the positi<strong>on</strong> <strong>of</strong> railing.<br />

Table 1: The Critical Wind Speed Varying With The Different Railing<br />

case porosity positi<strong>on</strong><br />

Flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed(m/s)<br />

-3° 0° +3°<br />

1 90% Initial positi<strong>on</strong> >74.6 73.0 61.3<br />

2 60% Initial positi<strong>on</strong> >75.3 57.6 44.8<br />

3 60% 5mm inside >74.8 58.6 42.4<br />

4 60% 10mm inside >76.2 57.9 44.0<br />

Figure2: Vortex Movement <strong>of</strong> Tacoma Deck<br />

Figure3: Vortex Movement <strong>of</strong> Box Girder


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

The Influence <strong>of</strong> Inspecti<strong>on</strong> Rail <strong>on</strong> Flutter Critical Wind Speed<br />

The <strong>aerodynamic</strong> stability <strong>of</strong> the girder may be sensitive to the distance between the<br />

rail top and the girder bottom (Y<strong>on</strong>gxin Yang et al., 2008). Three different kind <strong>of</strong> adjustment<br />

were carried out to investigate the potential influence. The distance was increased by 1mm<br />

and 3mm (prototype 5cm and 15cm) in the tests (the porosity <strong>of</strong> railing is 90%). Flutter<br />

critical speeds <strong>of</strong> these secti<strong>on</strong>s were measured and are summarized in table 2. It is found that<br />

the increase <strong>of</strong> distance is benefit to the critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed at 0°and -3°attack angle, but<br />

disadvantage to the <strong>aerodynamic</strong> stability <strong>of</strong> the girder at +3°attack angle. Because the<br />

dominant factor <strong>of</strong> <strong>aerodynamic</strong> stability is the minimum value am<strong>on</strong>g three critical <str<strong>on</strong>g>wind</str<strong>on</strong>g><br />

speeds, the increasing <strong>of</strong> distance is not a good choice to strengthen the <strong>aerodynamic</strong> stability<br />

<strong>of</strong> the girder.<br />

Table 2: The Critical Wind Speed Varying With The Change <strong>of</strong> Railway<br />

case<br />

distance<br />

Flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed(m/s)<br />

-3° 0° +3°<br />

Initial design 5mm from the bottom >79.0 73 61.3<br />

Increment 1mm 6mm from the bottom >81 >80 59.6<br />

Increment 3mm 8mm from the bottom >84 >82.5 58.1<br />

The Influence <strong>of</strong> Guide Wing <strong>on</strong> Flutter Critical Wind Speed<br />

The guide wing <strong>on</strong> the edge <strong>of</strong> sideway can smooth airflow while passing through the<br />

secti<strong>on</strong>. Hence the <strong>aerodynamic</strong> stability maybe strengthened (K. Wilde et al., 2001; S<strong>on</strong>g<br />

Jinzh<strong>on</strong>g et al., 2002; T. Miyata, 2003). Because <strong>of</strong> the particularity <strong>of</strong> deck c<strong>on</strong>figurati<strong>on</strong>, the<br />

optimized guide wing should be selected by intensive <str<strong>on</strong>g>wind</str<strong>on</strong>g> <str<strong>on</strong>g>tunnel</str<strong>on</strong>g> tests. Total nine different<br />

types <strong>of</strong> guide wings are applied in the tests, with different width and obliquity. The railing<br />

porosity is 60% for the secti<strong>on</strong> model in the tests. Flutter <str<strong>on</strong>g>wind</str<strong>on</strong>g> speeds were obtained in the<br />

tests for the secti<strong>on</strong> model with attack angle +3 deg and 0 deg, and the results are shown in<br />

Table 3.<br />

It is observed that the wider and the positive obliquity guide wing can improve the<br />

<strong>aerodynamic</strong> stability distinctly although the railing has low porosity. On the other hand, the<br />

guide wing will increase the complexity <strong>of</strong> the structure design and c<strong>on</strong>structi<strong>on</strong>, particularly<br />

in the locati<strong>on</strong> <strong>of</strong> rostra, and the maintenance cost will increase corresp<strong>on</strong>dingly. The guide<br />

wing <strong>of</strong> the deck is not recommended in the design unless there is no alternative means to<br />

improve the <strong>aerodynamic</strong> performance.<br />

Figure 4: Outline <strong>of</strong> Guide Wing


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

Table 3: The Critical Wind Speed Varying With Different Guide Wings<br />

case<br />

Guide wing Flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed(m/s)<br />

width obliquity 0° 3°<br />

1 50cm +15 52.2 44.9<br />

2 50cm 0 51.47 41.98<br />

3 50cm -42 54.75 42.34<br />

4 100cm +15 54.96 52.05<br />

5 100cm 0 52.78 50.23<br />

6 100cm -42 58.77 45.63<br />

7 125cm +15 60.23 63.88<br />

8 125cm 0 56.94 55.48<br />

9 125cm -42 62.78 49.64<br />

The Influence <strong>of</strong> Secti<strong>on</strong> Rostra <strong>on</strong> Flutter Critical Wind Speed<br />

Because the critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is sensitive to shape <strong>of</strong> secti<strong>on</strong> rostra (A. Larsen, 1993;<br />

S<strong>on</strong>g Jinzh<strong>on</strong>g et al., 2002; T. Miyata, 2003), rostra with different width and acutance is taken<br />

into account in the tests. The acutance varies from 57 deg to 25 deg, corresp<strong>on</strong>dingly the<br />

width varying from 1.9m to 3.3m. Total twenty-<strong>on</strong>e model cases were tested. The results are<br />

shown in table 4. It is noted that the flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed increases al<strong>on</strong>g with the<br />

increasing <strong>of</strong> rostra width and acutance. However, the flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed comes down<br />

distinctly when the width <strong>of</strong> rostra exceeds 3m. The mechanism for rostra with a width more<br />

than 3m may weaken the stability will be discussed in the later chapter.<br />

Table 4: The Critical Wind Speed Varying With Different Secti<strong>on</strong> Rostra<br />

Flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed(m/s)<br />

case Type <strong>of</strong> the secti<strong>on</strong> rostra<br />

+3° -3° -3°<br />

1 width:1.9m 51.5 >69.6 >70.6<br />

2 width:2.1m 53.7 >70.7 >70.3<br />

3 width:2.3m 54.6 >71.2 >70.5<br />

4 width:2.5m 56.7 >70.8 >71.2<br />

5 width:2.7m 58.6 >71.5 >75.2<br />

6 width:3.0m 63.4 >72.5 >70.9<br />

7 width:3.3m 59.3 >71.3 >72.8


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

64<br />

3m width<br />

62<br />

flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed (m/s)<br />

60<br />

58<br />

56<br />

54<br />

52<br />

3.3m width<br />

2.7m width<br />

2.5m width<br />

2.3m width<br />

2.1m width<br />

1.9m width<br />

50<br />

20 25 30 35 40 45 50 55 60<br />

the acutance <strong>of</strong> rostra (degree)<br />

Figure 5: Flutter Wind Speed Varying With The Acutance <strong>of</strong> Rostra<br />

The Influence <strong>of</strong> Steepness <strong>of</strong> Lower Inclined Web Slope <strong>on</strong> Flutter Critical Wind Speed<br />

The wider and acuminate secti<strong>on</strong> rostra are more difficult to be fabricated and fixed,<br />

implying more cost in design and c<strong>on</strong>structi<strong>on</strong>, although it can strengthen the <strong>aerodynamic</strong><br />

stability <strong>of</strong> the girder distinctly. Alternate way is to decrease the steepness <strong>of</strong> side wall slope,<br />

which can make the deck cross secti<strong>on</strong> more streamlined. When the slope decreases to 15°,<br />

see fig6, the flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is up to 67m/s, and it directly increases the flutter<br />

performance by 10%, and the width <strong>of</strong> secti<strong>on</strong> rostra is <strong>on</strong>ly 2.4m. The detailed test results are<br />

shown in table 5. The results also lead to an optimized secti<strong>on</strong> <strong>of</strong> girder: shorter rostra,<br />

without guide wing, low porosity railing. It also satisfies different kinds <strong>of</strong> requirements: high<br />

security, low cost, and more c<strong>on</strong>venience.<br />

case<br />

Table 5: The Critical Wind Speed (Slope Is 15°)<br />

Flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed(m/s)<br />

Secti<strong>on</strong> rostra<br />

-3° -3° -3°<br />

1 width:2.4m 67.1 >71.3 >73.5<br />

2 width:2.6m 62.0 >70.8 >72.7<br />

3 width:2.8m 61.1 >71.5 >72.4.<br />

Figure 6: The Lower Inclined Web Slope Decreased To 15°


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

The Discussi<strong>on</strong> <strong>on</strong> Mechanism <strong>of</strong> Aerodynamic Improvement<br />

According to the research results <strong>of</strong> airfoil (Abbott I. H., 1958), all classical airfoils<br />

are stalled at 16 deg. The lift is increasing with increasing attack angle, and <strong>on</strong>ce exceeding<br />

16 deg, the lift decreases, see figure 7. The flow detaches from the sucti<strong>on</strong> side and forms a<br />

vortex while the airfoils are stalled. Larsen based <strong>on</strong> the experience from vortex shedding<br />

tests (Larsen A. et al., 2000, 2008 ), found that the trapezoidal box secti<strong>on</strong>s was similar to the<br />

airfoils, and gave a c<strong>on</strong>clusi<strong>on</strong> that the flow al<strong>on</strong>g the bottom plate would stay mainly<br />

attached if lower inclined web angle α is less than approximately 16 deg. He also gave an<br />

example about the design <str<strong>on</strong>g>study</str<strong>on</strong>g> for a two span suspensi<strong>on</strong> bridge in Chile, whose lower<br />

inclined web angle is 14.8 deg, and no vortex-induced vibrati<strong>on</strong> was observed in the <str<strong>on</strong>g>wind</str<strong>on</strong>g><br />

<str<strong>on</strong>g>tunnel</str<strong>on</strong>g> testing. Another example was a new 1345 m suspensi<strong>on</strong> bridge in northern Norway,<br />

with 15.8 deg <strong>of</strong> lower side web angle, and the <str<strong>on</strong>g>wind</str<strong>on</strong>g> <str<strong>on</strong>g>tunnel</str<strong>on</strong>g> tests dem<strong>on</strong>strated that vortex<br />

induced vibrati<strong>on</strong> were absent. The c<strong>on</strong>trary examples were box girders <strong>of</strong> the Great Belt East<br />

Bridge and Osterøy Bridge, lower inclined web slope angles are 26.6° and 29.5°, respectively.<br />

Explicit vortex induced vibrati<strong>on</strong>s were observed for these bridges in full scale.<br />

Figure 7: The Lift Coefficient <strong>of</strong> Wings Varying With Attack Angle<br />

Similarly to a box secti<strong>on</strong> in the vortex shedding vibrati<strong>on</strong> status, in the flutter critical<br />

status, two vortices with counter directi<strong>on</strong> have also been observed at the both sides <strong>of</strong> the<br />

nose tail line <strong>of</strong> Great Belt East Bridge secti<strong>on</strong> through the PIV (Particle Image Velocimetry)<br />

technique(Zhang et al., 2009), which can give the girder enough momentum to increase its<br />

amplitude in a shot time and finally make the girder instable. When the <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is low,<br />

and under the flutter critical speed, the positive vortex blow the nose-tail line is more<br />

powerful than the above negative <strong>on</strong>e, the <strong>aerodynamic</strong> force is just a static lift force, see<br />

figure 8. When the <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is increasing, and close to the flutter critical speed, the<br />

negative vortex above the nose-tail line has been strengthen as powerful as the blow positive<br />

<strong>on</strong>e, and the <strong>aerodynamic</strong> force becomes to fluctuated force, see figure 9. If the frequency and<br />

the phase <strong>of</strong> the fluctuated force are close to bridge’s, the flutter <strong>of</strong> girder will be occur so<strong>on</strong>.<br />

In this paper, when the slope <strong>of</strong> the lower inclined web decreases to 15 deg(also less<br />

than 16 deg), there is a smaller dead air wake regi<strong>on</strong> below the nose-tail and the flow al<strong>on</strong>g<br />

the bottom plate will stay mainly attached the web, which making more difficult for formati<strong>on</strong><br />

<strong>of</strong> a large vortex. When the <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is increasing to the original flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed<br />

(former test girder with low critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed), because the little room gives the restrain to<br />

the forming <strong>of</strong> vortex, the counter vortices can’t give the girder powerful and efficient


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

excitati<strong>on</strong>. When the <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed increasing to a higher <strong>on</strong>e, the equalizati<strong>on</strong> counter vortices<br />

will form again at the similar positi<strong>on</strong> and the rhythmic excitati<strong>on</strong> is be back, which bring <strong>on</strong><br />

<strong>aerodynamic</strong> instability to the girder again.<br />

This explains can also be extended to interpret the results show in table4. When the<br />

slope <strong>of</strong> the lower inclined web is less than 16 deg, varying with the increasing <strong>of</strong> rostra width,<br />

there is a lager room for formati<strong>on</strong> <strong>of</strong> a large vortex, which is not propitious to the girder<br />

stability. In the tests, when the width <strong>of</strong> rostra exceeded 3m, there would be a larger room for<br />

formati<strong>on</strong> <strong>of</strong> a larger coherent vortex which made the flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed descend. Of<br />

course, this explains are also applicable to the interpretati<strong>on</strong> <strong>of</strong> results in table 5.<br />

Needing to point out is that the explain about the mechanism is based <strong>on</strong> the Larsen’s<br />

research <strong>on</strong> the vortex shedding vibrati<strong>on</strong> <strong>of</strong> Great Belt East Bridge, and Zhang’s research <strong>on</strong><br />

the flutter critical status <strong>of</strong> the same bridge by PIV technique, it <strong>on</strong>ly a assumpti<strong>on</strong> and a<br />

deducti<strong>on</strong> <strong>of</strong> <strong>aerodynamic</strong> improvement. Further more, it needs to be verified through the<br />

further <str<strong>on</strong>g>study</str<strong>on</strong>g> by the <str<strong>on</strong>g>wind</str<strong>on</strong>g> <str<strong>on</strong>g>tunnel</str<strong>on</strong>g> tests and CFD method in the future researches.<br />

Figure 8: Vortex Moment At The Low Wind Speed (Blow The Critical Speed)<br />

Figure 9: Vortex Moment At The High Wind Speed (Closing To Critical Speed)<br />

C<strong>on</strong>clusi<strong>on</strong>s<br />

The girders with high porosity railings have higher flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed than the<br />

<strong>on</strong>es with low porosity railings. The wider and acutance secti<strong>on</strong> rostra can strengthen the<br />

<strong>aerodynamic</strong> stability <strong>of</strong> the girder, but width can’t exceed 3m. The flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed<br />

is also sensitive to the steepness <strong>of</strong> blow inclined web slope. The lower is the slope, the higher


The Seventh Asia-Pacific C<strong>on</strong>ference <strong>on</strong> Wind Engineering, November 8-12, 2009, Taipei, Taiwan<br />

is <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed. When the slope <strong>of</strong> lower inclined web is less than 16 deg, the flutter critical<br />

<str<strong>on</strong>g>wind</str<strong>on</strong>g> speed <str<strong>on</strong>g>wind</str<strong>on</strong>g> will increasing dramatically.<br />

Through the <str<strong>on</strong>g>wind</str<strong>on</strong>g> <str<strong>on</strong>g>tunnel</str<strong>on</strong>g> tests, the final secti<strong>on</strong> has a good <strong>aerodynamic</strong> stability, and<br />

the flutter critical <str<strong>on</strong>g>wind</str<strong>on</strong>g> speed is up to 67.1m/s, and 79m/s in the later full scale <strong>aerodynamic</strong><br />

model tests. Of course, there is no vortex shedding vibrati<strong>on</strong> observed in the 1:50 and 1:20<br />

secti<strong>on</strong> model testing.<br />

References<br />

Allan Larsen, Aerodynamic aspects <strong>of</strong> the final design <strong>of</strong> the 1624m suspensi<strong>on</strong> bridge across the Great Belt,<br />

Journal <strong>of</strong> Wind Engineering and Industrial Aerodynamics,Volume 48, Issues 2-3, Oct.1993, Pages 261-285<br />

Toshio Miyata, Historical view <strong>of</strong> l<strong>on</strong>g-span bridge <strong>aerodynamic</strong>s, Journal <strong>of</strong> Wind Engineering and<br />

Industrial Aerodynamics 91 (2003) 1393–1410<br />

Bruno Luca, Mancini Giuseppe, Importance <strong>of</strong> Deck Details in Bridge Aerodynamics, Structural Engineering<br />

Internati<strong>on</strong>al, Volume 12, Number 4, 1 November 2002 , pp. 289-294(6)<br />

K. Wilde, P. Omenzetter, Y. Fujino, Suppressi<strong>on</strong> <strong>of</strong> bridge flutter by active deck-flaps c<strong>on</strong>trol system, J. Eng.<br />

Mech. 127 (1) (2001) 80–89.<br />

S<strong>on</strong>g Jinzh<strong>on</strong>g, Lin Zhixing, Xu Jianying, Research and Appliance <strong>of</strong> Aerodynamic Measure s about Wind<br />

resistance <strong>of</strong> Bridges, Journal Of T<strong>on</strong>gji University, Vol. 30 No. 5, May 2002<br />

Liu Cijun, Guo Zhenshan, Zhu Led<strong>on</strong>g, Influence <strong>of</strong> Railing Curbst<strong>on</strong>e Structure <strong>on</strong> Flutter Stability <strong>of</strong> Box<br />

Main Girder, Bridge C<strong>on</strong>structi<strong>on</strong>, 2008.02<br />

Y<strong>on</strong>gxin Yang, Yaojun Ge. Some Practices <strong>on</strong> Aerodynamic Flutter C<strong>on</strong>trol for L<strong>on</strong>g-Span Cable Supported<br />

Bridges, The 4 th Internati<strong>on</strong>al C<strong>on</strong>ference <strong>on</strong> AWAS’08, Jeju, Korea, 2008<br />

Abbott I. H. and V<strong>on</strong> Doenh<strong>of</strong>f A. E, Theory <strong>of</strong> Wing Secti<strong>on</strong>s, Dover Publicati<strong>on</strong>s, New York, 1958.<br />

Larsen. A., Esdahl, S., Andersen, J. E., Vejrum, T., Storebælt suspensi<strong>on</strong> bridge - vortex shedding excitati<strong>on</strong> and<br />

mitigati<strong>on</strong> by guide vanes. J. Wind Eng. Ind. Aerodyn.88 (2000), pp. 283-296.<br />

Larsen. A, Aerodynamic Stability and Vortex Shedding Excitati<strong>on</strong> <strong>of</strong> Suspensi<strong>on</strong> Bridges, The Keynote Paper<br />

<strong>of</strong> The 4 th Internati<strong>on</strong>al C<strong>on</strong>ference <strong>on</strong> AWAS’08, Jeju, Korea, 2008<br />

Zhang Wei, Ge Yaojun. Flow Field Mechanism <strong>of</strong> Wind Induced Vibrati<strong>on</strong> Resp<strong>on</strong>se <strong>of</strong> Large Span Bridge<br />

Influenced by Guide Vanes, China Journal <strong>of</strong> Highway and Transport, Vol.22 No. 3,May 2009

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