Page 26 - Global Tectonics
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THE INTERIOR OF THE EARTH  13



                                                                                 Compression
                                                                                        Nodal plane
                                                                    Auxiliary               Dilation
                                                                    plane



                                                           Fault plane  Focal sphere



                                                         Figure 2.5  Distribution of compressional and dilational
                                                         first arrivals from an earthquake on the surface of a

                                                         spherical Earth in which seismic velocity increases with
                                                         depth.


                                                         by considering the directions in which the seismic
            Figure 2.4  Quadrantal distribution of compressional   waves left the focal region, as it is apparent that com-

            and dilational P wave first motions about an   pressions and dilations are restricted to certain angular
            earthquake.                                  ranges.
                                                            A focal mechanism solution is obtained fi rstly  by
                                                         determining the location of the focus by the method
            defined by the fault plane and the auxiliary plane. No P   outlined in Section 2.1.4. Then, for each station record-

            waves propagate along these planes as movement of the   ing the earthquake, a model for the velocity structure
            fault imparts only shearing motions in their directions;   of the Earth is used to compute the travel path of the
            they are consequently known as nodal planes.  seismic wave from the focus to the station, and hence
               Simplistically, then, a focal mechanism solution   to calculate the direction in which the wave left the focal
            could be obtained by recording an earthquake at a   region. These directions are then plotted, using an
            number of seismographs distributed around its epicen-  appropriate symbol for compressional or dilational fi rst

            ter, determining the nature of the first motions of the   motion, on an equal area projection of the lower half
            P waves, and then selecting the two orthogonal planes   of the focal sphere, that is, an imaginary sphere of small
            which best divide compressional from dilational fi rst   but arbitrary radius centered on the focus (Fig. 2.5). An
            arrivals, that is, the nodal planes. In practice, however,   equal area net, which facilitates such a plot, is illustrated
            the technique is complicated by the spheroidal shape of   in Fig. 2.6. The scale around the circumference of such
            the Earth and the progressive increase of seismic veloc-  a net refers to the azimuth, or horizontal component of
            ity with depth that causes the seismic waves to follow   direction, while dips are plotted on the radial scale from
            curved travel paths between the focus and recorders.   0° at the perimeter to 90° at the center. Planes through
            Consider Fig. 2.5. The dotted line represents the con-  the focus are represented on such plots by great circles
            tinuation of the fault plane, and its intersection with the   with a curvature appropriate to their dip; hence a diam-
            Earth’s surface would represent the line separating   eter represents a vertical plane.
            compressional and dilational first motions if the waves   Let us assume that, for a particular earthquake, the

            generated by the earthquake followed straight-line   fault motion is strike-slip along a near vertical fault
            paths. The actual travel paths, however, are curved and   plane. This plane and the auxiliary plane plot as orthog-
            the surface intersection of the dashed line, correspond-  onal great circles on the projection of the focal sphere,

            ing to the path that would have been followed by a wave   as shown on Fig. 2.7. The lineation defined by the inter-
            leaving the focus in the direction of the fault plane,   section of these planes is almost vertical, so it is appar-
            represents the actual nodal plane.           ent that the direction of movement along the fault is
               It is clear then, that simple mapping of compres-  orthogonal to this intersection, that is, near horizontal.
            sional and dilational first motions on the Earth’s   The two shaded and two unshaded regions of the pro-

            surface cannot readily provide the focal mechanism   jection defined by the nodal planes now correspond to

            solution. However, the complications can be overcome   the directions in which compressional and dilational
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