Abstract

The abundance of wood in Brazil combined with the advantages of its use has lead to many studies focusing on optimizing the application of this raw material. In particular, stress-laminated-timber decks are an alternative to conventional building materials for short- to medium-span bridges, and its advantages include low weight and excellent flexibility that enable a high prefabrication rate and quick assembly on site. In order to make the best use of wood, this work studies the behavior of a stress-laminated-timber bridge deck using hardwoods. In brief, three different species were used as laminates, which with the prestress effect made it really difficult to have optimal precision in the numerical analysis, then resulting in higher displacements than those from the tests in almost all comparisons. However, the results of the experimental and numerical displacements followed the same pattern and linearity with reasonable values and low deflections, which demonstrates that the system worked as an orthotropic plate equivalent to the same deck system constructed out of conifers, as widely used in North America for such structures. Further research should be performed with one species only, so that even better results could be found.

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Acknowlegments

This study was financed in part by the Coordenação de Aperfeiçoamento de Pessoal de Nível Superior—Brasil (CAPES)—Finance Code 001.

Disclaimer

The authors declare that they are responsible for all content including text, images, tables, and others.

Notation

The following symbols are used in this paper:
C11
stiffness in the plane 1 and 1;
C12
stiffness in the plane 1 and 2;
C21
stiffness in the plane 2 and 1;
C22
stiffness in the plane 2 and 2;
C66
stiffness;
Ex
modulus of elasticity in direction x;
Ey
modulus of elasticity in direction y;
F
force of prestressing load (kN);
Gxy
shear modulus or transverse elastic modulus in the plane x and y;
G66
shear modulus or transverse elastic modulus;
L
length (m);
S11
flexibility in the plane 1 and 1;
S12
flexibility in the plane 1 and 2;
S21
flexibility in the plane 2 and 1;
S22
flexibility in the plane 2 and 2;
S66
flexibility;
Vyz
coefficient of Poisson;
X
bar reading (×10−6 cm/cm);
Y
load cell reading(N);
α
torsional parameter;
γxy
vector of tension in the plane x and y;
ɛ
reduced vector of deformations;
ɛx
vector of deformations in direction x;
ɛy
vector of deformations in direction y;
θ
flexural parameter;
σ
reduced vector of normal stress;
σx
vector of normal stress in direction y;
σy
vector of normal stress in direction y; and
τxy
vector of shear stress in the plane x and y.

References

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Published In

Go to Journal of Bridge Engineering
Journal of Bridge Engineering
Volume 26Issue 3March 2021

History

Received: Nov 21, 2019
Accepted: Aug 27, 2020
Published online: Jan 11, 2021
Published in print: Mar 1, 2021
Discussion open until: Jun 11, 2021

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Authors

Affiliations

Marcio Lima do Nascimento, Ph.D.
Dept. of Mathematics, Federal Univ. of Pará (UFPA), Belém 66075-110, Brazil.
Edson Fernando Castanheira Rodrigues, P.G.
Dept. of Civil Engineering (DECiv), Federal Univ. of São Carlos (UFSCar), São Carlos 13565-905, Brazil.
André Luis Christoforo, Ph.D.
Dept. of Civil Engineering (DECiv), Federal Univ. of São Carlos (UFSCar), São Carlos 13565-905, Brazil.
Francisco Antonio Rocco Lahr, Ph.D.
Dept. of Structural Engineering (SET), São Carlos Engineering School (EESC), São Paulo Univ. (USP), São Carlos 13566-590, Brazil.
Dept. of Structural Engineering (SET), São Carlos Engineering School (EESC), São Paulo Univ. (USP), São Carlos 13566-590, Brazil (corresponding author). ORCID: https://orcid.org/0000-0002-2544-3743. Email: [email protected]

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