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CT4860 STRUCTURAL DESIGN OF PAVEMENTS

CT4860 STRUCTURAL DESIGN OF PAVEMENTS

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3.4 Stresses and displacements due to traffic loadings<br />

3.4.1 Introduction<br />

In 1926 Westergaard published his original equations for the calculation of the<br />

maximum flexural tensile stress and the maximum vertical displacement due<br />

to a single wheel load in the interior, at the edge or at the corner of a single<br />

concrete slab. In latter years Westergaard himself as well as other<br />

researchers published several ‘modified’ Westergaard-equations. Until today<br />

this Westergaard-theory is widely used all over the world to calculate the<br />

stresses and displacements in concrete pavement structures due to traffic<br />

loadings. The Westergaard-theory is described in 3.4.2.<br />

In reality a concrete pavement structure does not exist of a single concrete<br />

slab, but of a number of concrete slabs with longitudinal and transverse joints<br />

(plain concrete pavements) or longitudinal joints and transverse cracks<br />

(reinforced concrete pavements). The load transfer in these joints and cracks,<br />

and the consequences for the stresses and displacements of the concrete<br />

pavement structure, are discussed in 3.4.3.<br />

3.4.2 Single concrete slab (Westergaard-theory)<br />

Westergaard developed a theory for the maximum stress (flexural tensile<br />

stress) and the maximum vertical displacement (deflection) due to a single<br />

wheel load, located in the interior (middle), along the edge or in a corner of a<br />

single (concrete) slab on an elastic foundation (springs with a stiffness equal<br />

to the modulus of substructure reaction k).<br />

The fully supported slab is assumed to be such large, that the edges and<br />

corners don’t have any significant influence on the maximum stress and<br />

deflection.<br />

In the cases that the single wheel load is in the interior or along the edge or<br />

crack of the concrete slab, both the flexural tensile stress and deflection are<br />

maximum at the bottom of the concrete slab in the load centre. In case of a<br />

single wheel load in the corner of the slab, the deflection is maximum exactly<br />

in the corner while the flexural tensile stress is maximum at some distance of<br />

the corner at the top of the concrete slab (figure 13).<br />

Figure 13. Loading positions in Westergaard’s theory.<br />

32

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