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400   CHAPTER 12



                           (a)
                           4 Ma  43 Ma  83 Ma 100 Ma   121 Ma     176 Ma













                           (b)
                           78 Ma  94 Ma  98 Ma 106 Ma  114 Ma     137 Ma













                                             0  Temperature (°C)  1846

           Figure 12.14  Sequences from numerical models, scaled approximately to the mantle, in which a plume grows from a
           thermal boundary layer. In (a) the viscosity is a function of temperature, and in (b) the viscosity also increases by a
           factor of 20 at 700 km depth. In (b) the plume slows and thickens through the 700 km discontinuity but then narrows
           and speeds up in the low viscosity upper layer (from Davies, 1999. Copyright © Cambridge University Press, reproduced
           with permission).






           core–mantle boundary. It has been estimated that a   African superswell although, as in the Pacifi c,  there
           major plume may be fed for 100 Ma from a volume of   are several potential deep mantle, or primary, plumes
           layer D″ only tens of kilometers thick and 500–1000 km   around it (Figs 5.7, 12.11c). This contrast is also
           in diameter.                                 refl ected in the marked difference in the seismic veloc-
             If major upwellings, such as those beneath south-  ity anomalies in the upper mantle beneath the two
           ern Africa and the south Pacific, reach the base of   areas (Plate 12.2b,d between pp. 244 and 245). The

           the transition zone they may well form a thermal   differing characteristics of the African and Pacifi c super-
           boundary layer at this depth from which  secondary   swells may arise from the fact that the south Pacifi c
           plumes may originate (Brunet & Yuen, 2000; Courtillot   upwelling is the remnant of the Cretaceous superplume
           et al., 2003). These would be relatively short-lived and   in this area (Section 5.7). The uplift of southern Africa
           without initial flood basalts but may well account for   was also initiated in the mid-Cretaceous, suggesting

           the hotspots on the south Pacific superswell such as   that major mantle upwellings or superplumes may

           the Society and Cook-Austral islands, Samoa, Pitcairn,   have a life cycle analogous to, and perhaps related
           and Caroline (Fig. 5.7) (Adam & Bonneville, 2005).   to, the life cycle of the assembly and break-up of
           By contrast, there are no plumes within the southern   supercontinents.
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