Technical Papers
May 6, 2022

Static Response Assessment of the Entire Suspension Bridge under Horizontal Transverse Live Load: An Analytical Calculation Method

Publication: Journal of Bridge Engineering
Volume 27, Issue 7

Abstract

Long-span suspension bridge is a flexible structure. When subjected to a horizontal transverse live load, its deck undergoes significant transverse bending deformation, jeopardizing traffic safety. This paper proposes an analytical calculation method for the static response of the entire suspension bridge with a horizontal transverse distributed live load applied to its deck. First, each component’s geometric configuration and internal force for the suspension bridge subjected only to a dead load are obtained. Next, their values under the action of horizontal transverse live load are treated as basic unknown parameters. Then, governing equations are established based on geometric compatibility conditions, conservation of unstrained length, and force balance conditions. The unknown parameters are derived by nonlinear programming, estimating the entire suspension bridge’s displacements and internal force response. The proposed analytical calculation method only considers the structural state of the suspension bridge before and after the action of the live load but not the intermediate process. Therefore, the complex problem of geometric nonlinearity involved in the stress calculation of the suspension bridge is precluded, and the calculation results are more accurate. Furthermore, the conventional treatment of all hangers as a continuous thin film is avoided. Instead, the effects of the following factors are analyzed: tower bending in the bridge-axis direction, tower torsion, hanger elongation, hanger inclination, and rigid body displacement of the deck in the bridge-axis direction. Finally, the feasibility and effectiveness of the method are verified by finite-element method (FEM) analysis of a suspension bridge with a main span of 548 m.

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Acknowledgments

The work described in this paper was financially supported by the National Natural Science Foundation of China under Grants 52078134 and 51678148, the Natural Science Foundation of Jiangsu Province (BK20181277), and the National Key R&D Program of China (Grant No. 2017YFC0806009), which are gratefully acknowledged.

Notation

The following symbols are used in this paper:
Ac
cross-sectional area of the main cable;
Ah
cross-sectional area of the hanger;
ai
catenary equation parameter of the ith segment in the main cable in the main span;
aL
catenary equation parameter of the left-side span;
bh
transverse distance from each hanger to the longitudinal centerline of the deck;
bs
transverse distance from the vertical support at the deck end to the longitudinal centerline of the deck;
bt
horizontal distance from each tower column to the central axis;
Cm,1 and Cm,2
postintegration constant terms of the deck’s bending moment;
Dm,1
constant term of indefinite integration;
dm
length of the mth segment of the deck;
Eb
elastic modulus of the deck;
Ec
elastic modulus of the main cable;
Eh
elastic modulus of the hanger;
ΔFL,y
horizontal reaction force of the left antiwind support;
ΔFL,z,d
vertical reaction force increment on the downstream side of the left end;
ΔFL,z,u
vertical reaction force increment on the upstream sides of the left end;
G
shear modulus of the deck;
Hi
horizontal component of the force in the ith segment of the main cable under the combined action of the dead and live loads;
HL,u
horizontal force component in the main cable upstream of the left-side span;
HL,d
horizontal force component in the main cable downstream of the left-side span;
H1,u
horizontal force component in the first catenary segment of the main cable upstream of the main span;
H1,d
horizontal force components in the first catenary segment of the main cable downstream of the main span;
Ip
polar moment of inertia of the deck;
Iy
bending moment of inertia of the deck about the z-axis;
Iz
bending moment of inertia of the deck in the vertical direction;
L1
horizontal projected length of the main cable in the left-side span;
li
horizontal distance between the two endpoints of the ith catenary segment of the main cable in the bridge-axis direction;
Pi,x
component of the hanger force Pi in the x-direction;
Pi,y
components of the hanger force Pi in the y-direction;
Pi,z
components of the hanger force Pi in the z-direction;
q
self-weight of the main cable per unit length;
Sc,i
unstrained length of the ith catenary segment of the main cable in the main span in the initial state;
Sc,L
unstrained length of the main cable in the left-side span in the initial state;
Sc,R
unstrained length of the main cable in the right-side span in the initial state;
Sh,i
unstrained length of the ith hanger in the initial state;
Xb,i
X-coordinate of the ith lower hanging point in the global coordinate system;
Xc,i
X-coordinate of the ith upper hanging point in the global coordinate system;
Yb,i
Y-coordinate of the ith lower hanging point in the global coordinate system;
Yc,i
Y-coordinate of the ith upper hanging point in the global coordinate system;
Zb,i
Z-coordinate of the ith lower hanging point in the global coordinate system;
Zc,i
Z-coordinate of the ith upper hanging point in the global coordinate system;
αi
included angle between the plane of the ith catenary location and the xoz plane;
η(x)
function produced by indefinite integration λ(x)dx, with the constant term excluded;
ϕi
included angle between the ith catenary at point Oi and the xoy plane;
φi
included angle between the projection of the hanger force Pi on the xoz plane and the z-axis (the vertical inclination angle);
ΔPi,y,d
increment of the horizontal component of the hanger force downstream at the location of xi;
ΔPi,y,u
increment of the horizontal component of the hanger force upstream at the location of xi;
ΔPi,z,d
vertical force increment in the ith hanger on the downstream;
ΔPi,z,u
vertical force increment in the ith hanger on the upstream;
δB
flexibility coefficient of the left tower in lateral bending;
δi+1
included angle between the i + 1st catenary at point Oi and the xoy plane;
ζB
flexibility coefficient of the left tower in torsion;
θi
included angle between the projection of the hanger force Pi on the yoz plane and the z-axis (the transverse inclination angle); and
v
longitudinal rigid body displacement of the deck.

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Go to Journal of Bridge Engineering
Journal of Bridge Engineering
Volume 27Issue 7July 2022

History

Received: Aug 2, 2021
Accepted: Mar 7, 2022
Published online: May 6, 2022
Published in print: Jul 1, 2022
Discussion open until: Oct 6, 2022

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Authors

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Associate Professor, Key Laboratory of Concrete and Prestressed Concrete Structures of the Ministry of Education, Southeast Univ., Nanjing 211189, China (corresponding author). ORCID: https://orcid.org/0000-0002-8272-1121. Email: [email protected]
Master’s Candidate, Key Laboratory of Concrete and Prestressed Concrete Structures of the Ministry of Education, Southeast Univ., Nanjing 211189, China. Email: [email protected]
Gen-min Tian [email protected]
Ph.D. Candidate, Key Laboratory of Concrete and Prestressed Concrete Structures of the Ministry of Education, Southeast Univ., Nanjing 211189, China. Email: [email protected]
Master’s Candidate, Key Laboratory of Concrete and Prestressed Concrete Structures of the Ministry of Education, Southeast Univ., Nanjing 211189, China. ORCID: https://orcid.org/0000-0002-0117-7620. Email: [email protected]

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