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SEA FLOOR SPREADING AND TRANSFORM FAULTS  77



            rapid overturn in the outer core will ensure that the   4.1.4  Sea floor spreading

            temperature at the core–mantle boundary is essentially
            uniform. The inferred temperature differences in the
                                                         In the early 1960s, Dietz (1961) and Hess (1962) had
            lower mantle, however, will give rise to a nonuniform
                                                         proposed that continental drift might be accomplished
            distribution of heat flux at the core–mantle boundary.

                                                         by a process that Dietz termed sea fl oor  spreading
            Anomalously cold material near the boundary will
                                                         (Section 1.2). It was suggested that new oceanic litho-
            steepen the temperature gradient and increase the heat
                                                         sphere is created by the upwelling and partial melting
            flow, whereas hotter material will decrease the gradient

                                                         of material from the asthenosphere at the ocean ridges.

            and heat flow. The new advances in computer simula-
                                                         As the ocean gradually grows wider with the progres-
            tions of the geodynamo make it possible to explore this
                                                         sive creation of lithosphere, the continents marginal to
            possibility. The initial results of such computations
                                                         the ocean are moved apart. The drift between North
            (Glatzmaier et al., 1999) are very interesting and encour-
                                                         America and Europe, for example, would have been
            aging in that different heat flow distributions do produce

                                                         accomplished by the gradual growth of the Atlantic
            significant changes in the reversal frequency and might

                                                         Ocean over the past 180 Ma. Since the Earth is not
            well explain the variations observed in Fig. 4.4.
                                                         increasing in surface area by any signifi cant  amount
               The results obtained from numerical simulations of
                                                         (Section 12.3), the increase in size of those oceans
            the geodynamo since the mid 1990s represent remark-

                                                         growing by sea floor spreading would be balanced by
            able breakthroughs in our modeling and understanding
                                                         the destruction of lithosphere at the same rate in
            of the possible origin of the Earth’s magnetic fi eld.
                                                         another, shrinking, ocean by subduction at deep sea
            However one has to bear in mind that, although the
                                                         trenches situated around its margins.
            physical formulation of these models is thought to be
                                                            The driving mechanism of these movements was
            complete, the parameters assumed are not in the range
                                                         believed to be convection currents in the sub-litho-
            appropriate for the Earth. This is because the comput-
                                                         spheric mantle (Fig. 1.5). These were thought to form
            ing power available is still not adequate to cope with the
                                                         cells in which mantle ascended beneath ocean ridges,
            spatial and temporal resolution that would be required
                                                         bringing hot material to the surface and giving rise to
            in the integrations.

                                                         new lithosphere. The flow then moved horizontally
                              6    Number of intervals per analysis = 50
                              5
                             Estimate of reversal rate λ  4 2  Cretaceous
                              3
                                                           superchron
                              1
                              0
                                 0   20     40    60    80    100   120   140   160
                                                Mid-age of sliding window (Ma)
            Figure 4.4  Estimated frequency of geomagnetic reversals over the past 160 Ma (redrawn from Merrill et al., 1996, with
            permission from Academic Press. Copyright Elsevier 1996).
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