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SEA FLOOR SPREADING AND TRANSFORM FAULTS  73



            4.1 SEA FLOOR                                magnetic and acid igneous and sedimentary rocks are
                                                         usually only weakly magnetic. A full account of the
            SPREADING                                    magnetic surveying method is given in Kearey  et  al.
                                                         (2002).
                                                            On land, magnetic anomalies reflect the variable

                                                         geology of the upper continental crust. The oceanic
                                                         crust, however, is known to be laterally uniform (Section
            4.1.1 Introduction                           2.4.4) and so unless the magnetic properties are hetero-
                                                         geneous it would be expected that marine magnetic

            By the late 1950s much evidence for continental drift   anomalies would reflect this compositional uniformity.
            had been assembled, but the theory was not generally
            accepted. Up to this time, work had concentrated upon

            determining the pre-drift configurations of the conti-  4.1.2 Marine magnetic
            nents and assessing their geologic consequences. The
            paths by which the continents had attained their present   anomalies
            positions had not been determined. In order to study
            the kinematics of continental drift it was necessary to   Magnetic surveying is easily accomplished, and mea-
            study the regions now separating once juxtaposed con-  surements have been carried out from survey vessels
            tinents. Consequently, at this time interest moved from   since the mid 1950s both on specific surveys and

            the continents to the intervening ocean basins.  routinely on passage to the locations of other oceano-
               Any kind of direct observation of the sea fl oor, such   graphic investigations.
            as drilling, dredging, or submersible operations, is time   A most signifi cant magnetic anomaly map (Fig. 4.1)
            consuming, expensive, and provides only a low density   was constructed after detailed surveys off the western
            of data. Much of the information available over oceanic   seaboard of North America (Mason & Raff, 1961; Raff &
            areas has therefore been provided by geophysical   Mason, 1961). The magnetic field was shown to be any-

            surveys undertaken from ships or aircraft. One such   thing but uniform, and revealed an unexpected pattern

            method involves measuring variations in the strength   of stripes defined by steep gradients separating linear

            of the Earth’s magnetic field. This is accomplished using   regions of high amplitude positive and negative anoma-
            either fluxgate, proton precession, or optical absorption   lies. These magnetic lineations are remarkably persis-

            magnetometers, which require little in the way of ori-  tent, and can be traced for many hundreds of kilometers.
            entation so that the sensing element can be towed   Their continuity, however, is interrupted at major oceanic

            behind the ship or aircraft at a sufficient distance to   fracture zones, where the individual anomalies are offset
            minimize their magnetic effects. In this way total fi eld   laterally by distances of up to 1100 km.
            values are obtained which are accurate to ±1 nanotesla   Subsequent surveys have shown that magnetic linea-
            (nT) or about 1 part in 50,000. Magnetometers provide   tions are present in virtually all oceanic areas. They are
            a virtually continuous record of the strength of the geo-  generally 10–20 km wide and characterized by a peak-
            magnetic field along their travel paths. These absolute   to-peak amplitude of 500–1000 nT. They run parallel to

            values are subsequently corrected for the externally   the crests of the mid-ocean ridge system (Chapter 6),
            induced magnetic field variations which give rise to a   and are symmetrical about the ridge axes (Fig. 4.2).

            diurnal effect, and the regional magnetic fi eld  arising   The source of these linear magnetic anomalies
            from that part of the magnetic field generated in the   cannot be oceanic layer 1, which is made up of non-

            Earth’s core. In theory the resulting magnetic anoma-  magnetic sediments. They cannot originate at a depth
            lies should then be due solely to contrasts in the mag-  corresponding to layer 3 as sources solely within this
            netic properties of the underlying rocks. The anomalies   layer would be too deep to generate the steep anomaly
            originate from the generally small proportion of ferro-  gradients. The source of the anomalies must there-
            magnetic minerals (Section 3.6.2) contained within the   fore be, at least in part, in oceanic layer 2. This con-
            rocks, of which the most common is magnetite. In   clusion is consistent with the basaltic composition of
            general, ultramafi c and mafi c rocks contain a high pro-  layer 2 determined by dredging and drilling (Section
            portion of magnetite and thus give rise to large mag-  2.4.6), since basalt is known to contain a relatively
            netic anomalies. Metamorphic rocks are moderately   high proportion of magnetic minerals. The magnetic
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