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OCEAN RIDGES  141



            extent of melting beneath such ridges (Section 6.9),   The relatively smooth axial topography of fast-
            small variations in mantle temperature and/or compo-  spreading ridges is characterized by an axial high, up to
            sition would lead to greater proportional changes   400 m in height and 1–2 km wide, and fault scarps with
            in  the volume of magma produced (Michael  et  al.,   a relief of tens of meters, the fault planes dipping either
            2003).                                       towards or away from the ridge axis. Active volcanism

                                                         is largely confined to the axial high, and the smooth
                                                         topography is thought to result from the high eruption
                                                         rate and the low viscosity of the magma. The axial high
            6.9 SHALLOW                                  appears to correspond to and to be supported by the
                                                         buoyancy of the axial magma chamber beneath. Studies
            STRUCTURE OF THE                             of major fault scarps and drill core from DSDP/ODP
                                                         drill hole 504B, all in Pacific crust, reveal that at depth

            AXIAL REGION                                 the lava fl ows dip towards the ridge axis at which they
                                                         were erupted and that the dikes beneath them dip away
                                                         from the ridge axis (Karson, 2002). This geometry indi-
                                                         cates a very narrow and persistent zone of dike intru-
            As noted above (Section 6.1), normal oceanic crust,   sion, and isostatic subsidence as the thickness of the lava

            that is, not formed in the vicinity of hot spots or   flow unit increases away from the point of extrusion
            transform faults, has a remarkably uniform seismic   (Section 6.10). This relatively simple structure of
            thickness of 7 ±  1 km if generated at a full spreading   the upper crust at the crests of fast-spreading ridges is
                               −1
            rate in excess of 20 mm a . For a homogeneous mantle   illustrated in Fig. 6.16.
            this implies a comparable thermal gradient beneath all   The shallow structure at the crests of slow-spreading
            such ridge crests, and a similar degree of partial   ridges is fundamentally different to that on fast-spread-
            melting of the mantle, which produces the uniform   ing ridges (Smith & Cann, 1993). As a result of less

            thickness of mafic crust. The essential uniformity of   frequent eruptions of magma and a cooler, more brittle
            the thermal regime beneath ridges is also implied by   upper crust, extension by normal faulting is more pro-
            the lithospheric age versus depth relationship (Section   nounced. The fault scarps have approximately 100 m of
            6.4). However, the rate at which magma is supplied to   relief and the fault planes dip towards the ridge axis.

            the crust will depend on the spreading rate. On fast-  Volcanism is essentially confined to the inner valley
            spreading ridges the magma supply rate is such that   fl oor, and at any one time appears to be focused along
            the whole crestal region at relatively shallow depth is   specific axis-parallel fissures, forming axial volcanic


            kept hot and a steady state magma chamber exists.   ridges 1–5 km wide and tens of kilometers in length. As
            Indeed the crust above the magma chamber would   these ridges move off axis, as a result of further accre-
            be even hotter and weaker but for the cooling effect   tion, they may be cut by the faults that ultimately form
            of hydrothermal circulation (Section 6.5). On slow-  the bounding scarps of the median valley. The spacing
            spreading ridges the lower rate of magma supply   of these bounding faults appears to be about one-third
            enables the crust to cool by conduction, as well as   to one-half of the width of the inner valley, that is,
            hydrothermal circulation, between injections of   several kilometers. Within the inner valley fl oor  the

            magma from the mantle. As a result the crust is   topography is fissured and cut by small throw normal
            cooler, and a steady state magma chamber cannot be   faults, the density of these features giving an indication
                                                    −1
            maintained. At spreading rates of less than 20 mm a    of its age. There is clear evidence of alternate phases of
            this conductive cooling between injections of magma   volcanic and tectonic (magmatic and amagmatic) exten-
            extends into the mantle and inhibits melt generation.   sion of the crust, as one would expect if there are tran-
            This reduces the magma supply, as well as the magma   sient magma chambers beneath, which supply discrete
            supply rate, and hence the thickness of mafi c  crust   packets of magma to the inner valley fl oor.
            produced, as observed on the Southwest Indian Ocean   Very slow-spreading ridges are characterized by thin
            and Gakkel ridges (Section 6.1). It also makes the   mafic crust and large regions of peridotite exposures

            existence of even transient magma chambers beneath   where the mantle appears to have been emplaced
            such ridges rather unlikely except beneath the volcanic   directly to the sea floor. However there are also mag-

            centers (Section 6.6).                       matic segments analogous to the second order
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