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THE INTERIOR OF THE EARTH  45



            and  ρ w ,  ρ m  the densities of water and the mantle,   surface compensation. Such loads include small topo-
            respectively.                                graphic features and variations in crustal density due,
               Note that as the elastic layer becomes more rigid, D   for example, to small granitic or mafi c bodies  within
            approaches infi nity, λ approaches zero, and the depres-  the crust. This more realistic model of isostatic com-
            sion due to loading becomes small. Conversely, as the   pensation, that takes into account the fl exural rigidity
            layer becomes weaker, D approaches zero, λ approaches   of the lithosphere, is referred to as  fl exural  isostasy

            infinity, and the depression approaches  h(ρ s   −  ρ w )/  (Watts, 2001).
            (ρ m  − ρ s) (Watts & Ryan, 1976). This is equivalent to
            Airy-type isostatic equilibrium and indicates that for
            this mechanism to operate the elastic layer and fl uid   2.11.5 Isostatic rebound
            substrate must both be very weak.
               It can be shown that, for oceanic lithosphere away   The equilibrium flexural response of the lithosphere to

            from mid-ocean ridges, loads with a half-width of less   loading is independent of the precise mechanical prop-
            than about 50 km are supported by the fi nite strength   erties of the underlying asthenosphere as long as it

            of the lithosphere. Loads with half-widths in excess   facilitates flow. However, the reattainment of equilib-
            of about 500 km are in approximate isostatic equilib-  rium after removal of the load, a phenomenon known
            rium. Figure 2.31 illustrates the equilibrium attained   as isostatic rebound, is controlled by the viscosity of the
            by the oceanic lithosphere when loaded by a sea-  asthenosphere. Measurement of the rates of isostatic
            mount (Watts  et al., 1975). Thus, as a result of its   rebound provides a means of estimating the viscosity

            flexural rigidity, the lithosphere has suffi cient internal   of the upper mantle. Fennoscandia represents an
            strength to support relatively small loads without sub-  example of this type of study as precise leveling surveys
                                                         undertaken since the late 19th century have shown that
                                                         this region is undergoing uplift following the melting of
                                                         the Pleistocene ice sheet (Fig. 2.32). The maximum
                                                         uplift rates occur around the Gulf of Bothnia, where
                                                                                          −1
                                                         the land is rising at a rate of over 10 mm a . Twenty
                                            D
                                           D             thousand years ago the land surface was covered by an
                                            D            ice sheet about 2.5 km thick (Fig. 2.32a). The lithosphere
                                                         accommodated this load by flexing (Fig. 2.32b), result-

                                                         ing in a subsidence of 600–700 m and a lateral displace-
                                                         ment of asthenospheric material. This stage currently
                                                         pertains in Greenland and Antarctica where, in Green-
                                                         land, the land surface is depressed by as much as 250 m
                                                         below sea level by the weight of ice. Melting of the ice
                                                         was complete about 10,000 years ago (Fig. 2.32c), and
                                                         since this time the lithosphere has been returning to its
                                                         original position and the land rising in order to regain
                                                         isostatic equilibrium. A similar situation pertains in
                                                         northern Canada where the land surface around Hudson
                                                         Bay is rising subsequent to the removal of an icecap.
                                                         The rate of isostatic rebound provides an estimate for
                                                                                        21
                                                         the viscosity of the upper mantle of 10  Pa s  (Pascal
             Figure 2.31  Interpretation of the free air anomaly of
                                                         seconds), and measurements based on world-wide
             the Great Meteor Seamount, northeast Atlantic Ocean,
             in terms of flexural downbending of the crust. A model   modeling of post-glacial recovery and its associated


                                       22

             with the flexural rigidity (D) of 6 × 10  N m appears best   oceanic loading suggest that this figure generally applies
                                                  −3
             to simulate the observed anomaly. Densities in Mg m .   throughout the upper mantle as a whole (Peltier &
             Arrow marks the position 30°N, 28°W (redrawn from   Andrews, 1976). Compared to the viscosity of water
                                                                                  3
                                                            −3
             Watts et al., 1975, by permission of the American   (10  Pa s) or a lava fl ow (4 × 10  Pa s), the viscosity of
             Geophysical Union. Copyright © 1975 American   the sub-lithospheric mantle is extremely high and its

             Geophysical Union).                         fluid behavior is only apparent in processes with a large
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