Smith's Elements of Soil Mechanics. Ian Smith

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Название Smith's Elements of Soil Mechanics
Автор произведения Ian Smith
Жанр Отраслевые издания
Серия
Издательство Отраслевые издания
Год выпуска 0
isbn 9781119750413



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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When water seeps from a soil of permeability k1 into a soil of permeability k2, the principle of the square flow net is no longer valid.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.

equation

      If the portion of the flow net in the soil of permeability k1 is square, then:

equation Schematic illustration of effect of variation of permeability on a flow net. (a) k2 gtgtgt k1. (b) k2 ltltlt k1. Schematic illustration of flow across an interface when the flow lines are at an angle to it.

      2.15.5 Refraction of flow lines at interfaces

      An interface is the surface or boundary between two soils. If the flow lines across an interface are normal to it, then there will be no refraction and the flow net appears as shown in Fig. 2.31. When the flow lines meet the interface at some acute angle to the normal, then the lines are bent as they pass into the second soil.

      Let f1 cut RR in B and f2 cut RR in A.

      Let h1 and h2 be the equipotentials passing through A and B, respectively, and let the head drop between them be Δh.

      With uniform flow conditions, the flow into the interface will equal the flow out. Consider flow normal to the interface.

      In soil (1):

equation

      Similarly, it can be shown that, in soil (2):

equation

      Now q1 = q2,

      (2.38)equation

      Exercises

      Exercise 2.1

      In a falling head permeameter test on a fine sand, the sample had a diameter of 76 mm and a length of 152 mm with a standpipe of 12.7 mm diameter. A stopwatch was started when h was 508 mm and read 19.6 s when h was 254 mm. The test was repeated for a drop from 254 to 127 mm and the time was 19.4 s.

      Determine an average value for k in m/s.

      Answer 1.5 × 10−4 m/s

      Exercise