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128   CHAPTER 6



           its shallowest point beneath the ridge crest, but extend-  of the Mid-Atlantic Ridge. In fact the region of
           ing to 350 km to the west and 150 km to the east of the   primary melt only underlies crust 2–3 Ma in age,
           ridge crest (Fig. 6.8). Both the velocity anomalies and   whereas the anomalous uplift of ridges extends out to
           electrical conductivity are consistent with 1–2% partial   crust of 70–80 Ma in age. Partial melt in the upper
           melting (Evans et al., 1999). There is an indication of   mantle may therefore account for some of the uplift
           incipient melting to a depth of 180 km. The asymmetry   of ridge crests but cannot account for the uplift of
           of the region of partial melting is thought to be due to   ridge fl anks.
           a combination of two effects. Within the hot spot

           framework the western flank of the ridge is moving at

           more than twice the rate of the eastern flank (Fig. 6.8).
           It is also close to the South Pacifi c superswell (Section   6.4 DEPTH–AGE

           12.8.3). Enhanced upwelling and hence flow in the
           asthenosphere from the superswell and viscous drag   RELATIONSHIP

           beneath the fast moving Pacific plate are thought to

           produce higher rates of flow and hence higher tem-
           peratures beneath the western flank of the ridge. These  OF OCEANIC

           elevated temperatures are reflected in shallower

           bathymetry (Section 6.4) and a higher density of sea- LITHOSPHERE
           mount volcanism on the western flank compared to the

           eastern fl ank.
             The width of the region of partial melt defi ned by   The major factor contributing to the uplift of mid-
           the MELT experiment seems to be quite wide. One   ocean ridges is the expansion and contraction of the
           must recall however that the spreading rate at this   material of the upper mantle. As newly formed
           point is very high, fi ve times higher than that on much   oceanic lithosphere moves away from a mid-ocean


                                                Distance from axis (km)
                             West  400      200        0        200      400  East
                               101 mm yr  1                Crust       45 mm yr  1
                                0


                                           Primary               Lithospheric
                                           melting                 mantle
                              100        Incipient  E
                            Depth (km)  200  melting




                              300


                              400              410 km Discontinuity


           Fig. 6.8  Schematic cross-section beneath the East Pacific Rise at 17°S illustrating the extent of partial melting in the
           mantle deduced from the results of the MELT experiment. Plate velocities are in the hot spot reference frame. The
           region labeled E (embedded heterogeneity) indicates enhanced melting due to anomalously enriched mantle

           or localized upwelling (modified from MELT seismic team, 1998, Science 280, 1215–18, with permission from the
           AAAS).
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