Page 223 - Geotechnical Engineering Soil and Foundation Principles and Practice
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Pore Water Pressure, Capillary Water, and Frost Action
                218   Geotechnical Engineering









                 Figure 11.6
                 Annular ring of water linking two soil particles. The main attractive force is not from surface tension
                 but from the negative pore pressure created by the surface tension.





                                    water, whereas the convex radius tends to increase it. As the concave radius is
                                    smaller, the net effect is a decrease in pressure that pulls the grains together.

                                    The equation for negative pressure in this case uses the Laplace function to define
                                    the surface:

                                              1   1
                                      u ¼ T     þ                                                  ð11:10Þ
                                              r 1  r 2

                                    in which r 1 and r 2 are radii of curvature of a warped surface where it intersects two
                                    orthogonal principal planes. The expression in the parentheses is called the total
                                    curvature of the surface. A negative radius creates a positive pore pressure, so in
                                    Fig.11.5, r 1 , the internal radius of the ring of water, increases pressure in the water
                                    and therefore is negative.

                                    The negative pore pressure in capillary water therefore equals the surface tension
                                    of the water times the total curvature of the meniscus or air-water interface.
                                    This relationship is important because, as the moisture content changes, both
                                    radii of curvature also change.

                                    The influence of total curvature is illustrated in Fig. 11.7, where it will be seen
                                    that, if the moisture content increases such that the outer surface of the annular
                                    ring of connecting water becomes straight-sided (Fig. 11.7(a)), r 1 is infinite so its
                                    reciprocal makes no negative contribution to pore water pressure, which therefore
                                    is positive.
                                    When a soil is dried (Fig. 11.7(b)), the smaller radius is positive so pore pressure
                                    becomes negative. Opposing this tendency is the cross-sectional area of the ring
                                    of water as the soil dries out (Fig. 11.7(c)), which eventually will result in a net
                                    decrease in attraction between the two particles. Finally, r 1 can become so small
                                    that the negative pressure equals the vapor pressure of water, causing the soil to
                                    spontaneously dry out. This does not occur in clay because its adsorptive
                                    properties permit a high negative pressure. When sand dries it crumbles whereas
                                    a clay keeps getting stronger.

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