Smith's Elements of Soil Mechanics. Ian Smith

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      2.15.3 Permeability of sedimentary deposits

      A sedimentary deposit may consist of several different soils and it is often necessary to determine the average values of permeability in two directions, one parallel to the bedding planes and the other at right angles to them.

       Let there be n layers of thicknesses H1, H2, H3, … Hn.

       Let the total thickness of the layers be H.

       Let k1, k2, k3, … kn be the respective coefficients of permeability for each individual layer.

       Let the average permeability for the whole deposit be kx for flow parallel to the bedding planes, and kz for flow perpendicular to this direction.

      Consider flow parallel to the bedding planes:

equation

      where A = total area and i = hydraulic gradient.

      This total flow must equal the sum of the flow through each layer, therefore:

equation equation

      hence

      (2.34)equation

      Considering flow perpendicular to the bedding planes:

equation

      Considering unit area:

equation

      Now

equation

      where h1, h2, h3, etc., are the respective head losses across each layer.

      Now

equation

      hence

      (2.35)equation

      Beneath the fine silt layer, there is a stratum of water‐bearing gravel with a water pressure of 155 kPa. The surface of the sand is flooded with water to a depth of 1 m.

       Solution:

equation

      Taking the top of the gravel as datum:

      Head of water due to artesian pressure = 15.5 m

      Head of water due to groundwater = 3 × 4 + 1 = 13 m

      Therefore, excess head causing flow = 15.5 − 13 = 2.5 m.

equation

      This quantity of flow is the same through each layer.

      Excess head loss through fine silt:

equation

      Therefore,

equation

      Excess head loss through coarse silt:

equation

      Excess head loss through fine sand:

equation

      Excess head at interface between fine and coarse silt

equation

      Excess head at interface between fine sand and coarse silt

equation

      2.15.4 Seepage through soils of different permeabilities

      When water seeps from a soil of permeability k1 into a soil of permeability k2, the principle of the square flow net is no longer valid. If we consider a flow net in which the head drop across each figure, Δh, is a constant then, as has been shown, the flow through each figure is given by the expression:

      (2.36)equation

      If Δq is to remain the same when k is varied, then b/l must also vary. As an illustration of this effect, consider the case of two soils with k1 = k2/3.

      Then

equation

      and

      (2.37)equation

      i.e.

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