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234   CHAPTER 8




             In northern California, earthquakes reveal the pres-  plate velocity, those on the Pacific plate move toward
           ence of a  ∼120-km-wide zone of faulting within the   the northwest. The observed velocities vary smoothly


           Coast Ranges between the Pacific plate on the west and   across the San Andreas Fault. Two profiles (Fig. 8.19b)
           the Great Valley–Sierra Nevada microplate on the east   (gray shaded areas) show similar total velocity changes
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           (Fig. 8.18a). In this region, horizontal velocities (Fig.   of ∼42 mm a  but distinctly different velocity gradients.

           8.18b) show an approximately uniform distribution of   Along the northern profile, the fault-parallel velocity
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           right lateral motion toward N29°W (Savage  et al.,   drops by ∼30 mm a  across the San Andreas Fault and
           2004a). This direction is close to the local strike (N34°W)   decreases slightly through the San Joaquin Valley before
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           of the San Andreas Fault and results in dominantly   distributing some 12 mm a  across the Eastern Califor-
           strike-slip motion along the major faults in the area. A   nia Shear Zone. By contrast, the southern profi le shows
           velocity profile along a great circle passing through the   a total velocity drop across a distance that is about 50%

           Pacific–North America pole of rotation (Fig. 8.18c)   that in the northern profi le. This reflects the difference


           illustrates this result by showing the components of   in the geometry of the fault system from north to
           motion that occur parallel to and perpendicular to the   south. The flat portion of the northern profi le mirrors

           trace of the San Andreas Fault. Slip rates parallel to the   the relative stability of the ∼200-km-wide Great Valley–
           fault are highest. Other faults display lower rates. In   Sierra Nevada microplate, with the deforming central
           addition, the westward movement of the Great Valley–  segment of the San Andreas Fault to the west and
           Sierra Nevada block relative to the Pacifi c plate (Dixon   Eastern California Shear Zone to the east. By contrast,
           et al., 2000; Williams et al., 2006) and the slight obliquity   the southern profile shows that the 40-km-wide zone

           between this motion and the trace of the San Andreas   between the San Andreas and San Jacinto faults accom-
           Fault (Prescott et al., 2001; Savage et al., 2004a) produces   modates approximately 80% of the relative plate
           a small component of contraction across the Coast   motion.
           Ranges. This latter result is supported by both geologic   North of the Garlock Fault, relative motion is
           data (Fig. 8.7b, inset) and by earthquake focal mecha-  deflected east of the Sierra Nevada by deformation in

           nisms that show thrust solutions west of the Great   the southern Walker Lane (Figs 7.9, 8.1). This eastward

           Valley (Fig. 7.10). By contrast, little deformation occurs   defl ection reflects an extensional step-over between the
           across the Great Valley and within the Sierra Nevada,   northwest-trending faults of the Eastern California
           suggesting that these regions form a coherent, rigid   Shear Zone and those located along the eastern margin
           block.                                       of the Sierra Nevada (Oldow, 2003). North of the step-
             In southern California, the distribution of earth-  over, the zone of deformation broadens into the central
           quakes indicates that relative plate motion is accom-  and northern Walker Lane and central Nevada seismic
           modated across a zone that is several hundreds of   belt (Fig. 8.20a). Earthquake focal mechanisms (Fig.
           kilometers wide (Fig. 7.8). South of latitude 34°N,   7.10) indicate that displacements in these latter belts
           some motion is distributed between the San Jacinto and   involve both strike-slip and normal fault motion on vari-
           San Andreas faults (Fig. 8.1). Becker et al. (2005) esti-  ably oriented faults. Horizontal velocities increase from
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           mated that the former accommodates some 15 mm a    2–3 mm a  to ∼14 mm a  from the central Great Basin
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           of slip and the latter ∼23 mm a . Within the Transverse   (Section 7.3) toward the Sierra Nevada (Oldow, 2003).
           Ranges, where crustal shortening and surface uplift   Accompanying this rate increase, the directions of
           accommodate a component of the motion (Fig. 8.8),   motion rotate clockwise from west-northwest to north-
           slip on the San Andreas Fault appears to be signifi cantly   west (Fig. 8.20b), indicating an increase in a component
           slower (Meade & Hager, 2005). Other displacements   of dextral strike-slip deformation from east to west.
           occur along major sinistral faults, such as the Garlock,   Oldow (2003) showed that two distinctive zones of
           Raymond Hill, and Cucamonga faults (Fig. 8.8a), and   transtension characterize this belt: one that is domi-
           by the clockwise and anticlockwise rotation of crustal   nated by extension on the west (domain III) and another
           blocks about vertical axes (Savage et al., 2004b; Bos &   that is dominated by strike-slip motion on the east
           Spakman, 2005).                              (domain II in Fig. 8.20b). Together with deformation in
             Figure 8.19a shows an example of a velocity fi eld for   the central and eastern Basin and Range (Section 7.3),
           southern California in a local reference frame (Meade   these belts accommodate up to 25% of the relative
           & Hager, 2005). Stations on the North American plate   motion between the Pacific and North American plates

           move toward the southeast at about half of the relative   (Bennett  et al., 1999). This transfer of motion east of
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