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4.6 Gravitational compaction of a hydrostatic clay layer  91

            the effective stress is then given by equation (4.63). The vertical effective stress under
            hydrostatic conditions is given by

                                           z

                                    σ =    (  −   f )g(1 − φ) dz               (4.67)
                                         0
            where the z-axis is pointing downwards and the surface of the layer is z = 0. The inte-
            gral (4.67) is not trivial to carry out in the z-coordinate, because the porosity is not yet
            known as a function of z. The trick is now to switch to the Lagrangian coordinate defined
            by the position in the layer measured as net (porosity-free) rock above the base of the layer.
            This is the so-called ζ-coordinate, and we have that dζ = (1 − φ)dz.(The ζ-coordinate
            was introduced in Section 3.17.) The vertical effective stress under hydrostatic conditions
            is therefore
                                                    ∗

                                      σ = (  −   f )g(ζ − ζ)                   (4.68)
            where ζ  ∗  is the ζ-coordinate for the top of the layer. We then get that the normal
            consolidation line (4.63)asafunctionofthe ζ-coordinate is
                                                    ∗
                                                   ζ − ζ
                                     e = e 0 − C v ln                          (4.69)
                                                     ζ 0

            where ζ 0 = σ /((  −   f )g) is the reference ζ-thickness that corresponds to σ . We would

                       0                                                  0
            like to have the void ratio as a function of z rather than ζ, and a step in that direction is to
            have the z-coordinate as a function of ζ too. The z-coordinate is given by equation (3.153):
                                                    ∗
                                     ζ  ∗  dζ       ζ
                               z =             =      1 + e(ζ) dζ.             (4.70)
                                   ζ   1 − φ(ζ)   ζ
            This integration is straightforward to carry out and the z-coordinate as a function of the
            ζ-coordinate is
                                                         
 ∗

                                                          ζ − ζ
                                  ∗
                             z = (ζ − ζ) 1 + e 0 + C v − C v ln   .            (4.71)
                                                            ζ 0
            Notice that both the void ratio (4.69) and the z-coordinate (4.71) are only functions of the
                                  ∗
            ζ-depth from the surface ζ − ζ. The void ratio can now be plotted as a function of the
            z-coordinate by combining equations (4.69) and (4.71), since both equations are parame-
            terized by the ζ-coordinate. Figure 4.3 shows the porosity of a clay layer as a function of
                                                                              4

            depth (z-coordinate) when C v = 0.2, e 0 = 1.5, σ = 1 kPa and (  −   f )g = 10 Pa/m.
                                                    0
            With these data we get that ζ 0 = 1m.

            Exercise 4.6 Derive equation (4.71). Hint:  ln x =−x + x ln x.
            Exercise 4.7 Equation (4.69) for the normal consolidation line and equation (4.71)for the
            z-coordinate can be extended with a surface load σ L . The equation for the void ratio is then
                                                ζ − ζ    σ L
                                                  ∗
                                   e = e 0 − C v ln    +                       (4.72)
                                                  ζ 0    σ
                                                          0
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