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Analysis of numerical models of an integral bridge resting on an elastic half-space Cover

Analysis of numerical models of an integral bridge resting on an elastic half-space

Open Access
|Dec 2024

Figures & Tables

Figure 1:

Analyzed integral bridge.

Figure 2:

Soil layer used in numerical models A and C.

Figure 3:

Finite element mesh of complex models A and C.

Figure 4:

Finite element mesh of simple model B.

Figure 5:

Location of the applied springs under the footing foundations in simple model B.

Table 1:

Spring constants.

ElementPier footingAbutment footing
βx (L/B)L=8 m, B=4 mL=10 m, B=3 m
βx =0.944βx =0.976
βy (L/B)L=4 m, B=8 mL=3 m, B=10 m
βy =1.012βy =1.096
βz (L/B)L=4 m, B=8 mL=3 m, B=10 m
βz =2.175βz =2.3
βφx (L/B)L=4 m, B=8 mL=3 m, B=10 m
βφx =0.435βφx =0.402
βφy (L/B)L=8 m, B=4 mL=10 m, B=3 m
βφy =0.595βφy =0.721
kx (kN/m)427,021427,819
ky (kN/m)457,832480,236
kz (kN/m)560,860574,345
kφx (kN/m/rad)2,540,6261,650,517
kφy (kN/m/rad)6,944,4379,854,189
Table 2:

Material properties used in the analysis.

ModelA, B, C
SoilLoose sand and gravel [27]
Es (MN/m2)80 (Middle range value)
ν0.35
ϕ40 (model A)
G (MN/m2)30.8
L (m)3 and 4
B (m)10 and 8
Bridge structureConcrete C50/60
Ecm (MN/m2)37,000
ν0.2

[i] where: E – modulus of elasticity, ν – Poisson’s ratio, ϕ – the soil’s internal angle of friction, G – the soil’s shear modulus, L – length of the foundation (in the plane of rotation for the case of rocking), and B – width of the foundation (along the axis of rotation for the case of rocking).

Table 3:

Load applied to the structure.

Load typeValue
SW of the bridge structure SW24 kN/m3
UDL 110 kN/m2
UDL 225 kN/m2
The characteristic value of the maximum expansion range of the uniform bridge temperature component∆TN,exp=36°C

[i] SW: self-weight, UDL: uniform distributed load

Table 4:

Equations for spring constants for a rectangular footing [21], [22].

Spring constantsMotionReference
Vertical stiffnessgraphic/j_sgem-2024-0026_ingr_001.pngBarkan (1962)
(3.1)
kz=G1νβzBL
Horizontal stiffnessgraphic/j_sgem-2024-0026_ingr_002.pngBarkan (1962)
(3.2)
ky=21+νGβyBL
Rocking stiffnessgraphic/j_sgem-2024-0026_ingr_003.pngGorbunov-Posadov (1961)
(3.3)
kϕ=G1νβϕBL2

[i] where: L – length of foundation (in the plane of rotation for the case of rocking), B – width of foundation (along the axis of rotation for the case of rocking), ν – the soil’s Poisson’s ratio, G – the soil’s shear modulus, (βy, βz, βϕ) – spring coefficients, and (ky, kz, kϕ) – spring constants.

Figure 6:

Actual soil deformation and according to the theory of elasticity.

Figure 7:

Bending moments in piers C1 and C2 where A and C are complex bridge models and B is a simple bridge model.

Figure 8:

Shear and axial forces in piers C1 and C2.

Figure 9:

Horizontal and vertical displacements in piers C1 and C2 where Ux and Uy are horizontal displacements along the X-axis and Y-axis direction and Uz is the vertical displacement along the Z-axis direction.

DOI: https://doi.org/10.2478/sgem-2024-0026 | Journal eISSN: 2083-831X (formerly 0137-124X) | Journal ISSN: 0137-6365
Language: English
Page range: 337 - 348
Submitted on: Apr 17, 2024
Accepted on: Nov 11, 2024
Published on: Dec 22, 2024
Published by: Wroclaw University of Science and Technology
In partnership with: Paradigm Publishing Services

© 2024 Andrzej Helowicz, published by Wroclaw University of Science and Technology
This work is licensed under the Creative Commons Attribution 4.0 License.