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Deformation behaviour of railway embankment ... - Liikennevirasto

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17<br />

2 INTRODUCTION TO THE MECHANICAL BEHAVIOUR OF GRANULAR<br />

MATERIALS<br />

2.1 Stresses in engineering materials<br />

The stress state acting on a given infinitesimal cubic soil element can be defined by its<br />

normal and shear stress components oriented according to a cartesian reference system,<br />

as illustrated in Figure 2.1:1.<br />

Figure 2.1:1 Stress components on a cubic soil element.<br />

The stress components are <strong>of</strong>ten given in a matrix form. Stress is a tensor which can be<br />

represented by a matrix in Cartesian coordinates:<br />

σ<br />

τ<br />

xx<br />

yx<br />

zx<br />

τ<br />

τ<br />

xy<br />

yy<br />

zy<br />

τ<br />

σ<br />

xz<br />

σ = τ σ τ . (Eq. 2.1:1)<br />

yz<br />

zz<br />

The indices refer to the coordinate system x, y, z. The first index specifies the direction<br />

in which the stress component acts, and the second identifies the orientation <strong>of</strong> the<br />

surface upon which it is acting.<br />

We can use equilibrium <strong>of</strong> moments to study the relationship between τ xy and τ yx .<br />

Assuming a unit thickness, the horizontal and vertical faces are <strong>of</strong> area dx and dy<br />

respectively (Figure 2.1:2).

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