2017
DOI: 10.1016/j.cnsns.2016.05.028
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Torsional instability in suspension bridges: The Tacoma Narrows Bridge case

Abstract: All attempts of aeroelastic explanations for the torsional instability of suspension bridges have been somehow criticised and none of them is unanimously accepted by the scientific community. We suggest a new nonlinear model for a suspension bridge and we perform numerical experiments with the parameters corresponding to the collapsed Tacoma Nar- rows Bridge. We show that the thresholds of instability are in line with those observed the day of the collapse. Our analysis enables us to give a new explanation for… Show more

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Cited by 59 publications
(56 citation statements)
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“…The collapse occurred after four months of use. According to Hobbs (2006) [31], Arioli and Gazzola (2017) [32], the principal cause of the collapse are the excessive dynamic torsional oscillations resulting from the vortex shedding. The study of this bridge's collapse was facilitated by the felicitous fact that the bridge behavior could be precisely monitored, from the start of the collapse to the crash moment, by filming that registered the oscillations and the nature of destruction.…”
Section: Resultsmentioning
confidence: 99%
“…The collapse occurred after four months of use. According to Hobbs (2006) [31], Arioli and Gazzola (2017) [32], the principal cause of the collapse are the excessive dynamic torsional oscillations resulting from the vortex shedding. The study of this bridge's collapse was facilitated by the felicitous fact that the bridge behavior could be precisely monitored, from the start of the collapse to the crash moment, by filming that registered the oscillations and the nature of destruction.…”
Section: Resultsmentioning
confidence: 99%
“…Theorem 13 states that small periodic forcing terms (such as small vortex shedding) generate a stable prevailing mode of oscillation to which all the solutions approach as t increases. But since each periodic movement (or mode of oscillation) has its own threshold of instability, see [9,19,25,27], it is more realistic to address the following fluid-structure interaction problem.…”
Section: Theorem 12 ([237]mentioning
confidence: 99%
“…Following Definition 1, we put w 0 k := 2 L w 0 k , w 1 k := 2 L w 1 k and similarly for the θ initial conditions. Applying a similar procedure to [6,7] we excite one single longitudinal mode (the j th ) at a time, applying an initial condition 10 −3 smaller on all the other components, i.e. in dimensionless form…”
Section: Numerical Experimentsmentioning
confidence: 99%
“…We consider an isolated model aiming to show that the origin of the torsional instability is purely structural, as proposed in other works [5,6,7]; in particular we suppose that the wind introduces energy in the structure, exciting one longitudinal mode at a time, through the initial conditions. This is legitimate since the frequency of the vortex shedding usually excites one mode.…”
Section: Introductionmentioning
confidence: 99%