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THE FRAMEWORK OF PLATE TECTONICS  113



            necessary information, from oceanic magnetic anoma-  ment of the Alpine Fault of New Zealand (Fig. 5.19c),
            lies and fracture zones, is available.       which is a dextral transform fault linking the Tonga-
                                                         Kermadec Trench, beneath which Pacifi c lithosphere is
                                                         underthrusting in a southwesterly direction, to a trench
            5.10 STABILITY OF                            to the south of New Zealand where the Tasman Sea is
                                                         being consumed in a northeasterly direction (McKenzie
            TRIPLE JUNCTIONS                             & Morgan, 1969).
                                                            A more complex and potentially unstable situation
                                                         arises when three plates come into contact at a triple
                                                         junction. Quadruple junctions are always unstable, and
            The stability of the boundaries between plates is depen-  immediately devolve into a pair of stable triple junctions,
            dent upon their relative velocity vectors. If a boundary   as will be shown later.
            is unstable it will exist only instantaneously and will   The Earth’s surface is covered by more than two
            immediately devolve into a stable confi guration.  plates, therefore there must be points at which three
               Figure 5.19a shows an unstable boundary between   plates come together to form triple junctions. In a
            two plates where plate X is underthrusting plate Y at bc   similar fashion to a boundary between two plates, the
            in a northeasterly direction and plate Y is underthrust-  stability of triple junctions depends upon the relative
            ing plate X at ab in a southwesterly direction. The   directions of the velocity vectors of the plates in
            boundary is unstable because a trench can only consume   contact. Figure 5.20 shows a triple junction between a
            in one direction, so to accommodate these movements   ridge (R), trench (T), and transform fault (F). From this

            a dextral transform fault develops at b (Fig. 5.19b). This   figure it can be appreciated that, in order to be stable,
            sequence of events may have occurred in the develop-  the triple junction must be capable of migrating up or




































            Figure 5.19  (a,b) Evolution of a trench. (c) Alpine Fault of New Zealand (redrawn from McKenzie & Morgan, 1969, with
            permission from Nature 224, 125–33. Copyright © 1969 Macmillan Publishers Ltd).
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