Ar/
Ar plateau ages for selected field reversals,
Geophys. Res. Lett., 20, 1607-1610, 1993.
Ar/
Ar dating
of the Brunhes-Matuyama geomagnetic field reversal, Science, 256, 356-357, 1992.
-10
30'N: Evolution
of ridge segments and discontinuities from SeaMARC II and three-dimensional magnetic
studies, J. Geophys. Res., 97, 6959-6982, 1992.
-27
30'S) from Sea Beam and magnetic data, J. Geophys. Res., 97,
6983-7010, 1992.
Figure 1:
Non-rigorous comparison of 148 geodesic rates derived from
SLR or VLBI measurements at 20 sites on five plates (Australia, Eurasia,
Nazca, North America, and Pacific) [ Smith et al., 1992] and geodesic
rates predicted by NUVEL-1A. The solid line represents the slope and
intercept of the best, least-squares fit to the two sets of rates weighted
by their uncertainties. Dotted line has a slope of 1.0 and intercept of
0.0, corresponding to perfect agreement between the two sets of rates.
Dashed line shows the geodesic rates predicted by NUVEL-1, which are
4.38% faster than rates predicted
Figure 1. (continued):
by NUVEL-1A. A rigorous comparison
of the observed and predicted geodesic rates would incorporate the
variances and covariances for both sets of rates. The non-zero intercept,
which implies an absolute offset of
1 millimeter per year between
the observed and predicted rates, may reflect the still limited number
of plates and sites sampled by SLR or VLBI.
Figure 2: Upper---Microplate model based on a simple, concentrically
rotating bearing. Bold dark lines show positions of major spreading
centers, overlapping about the microplate. Stippled regions show areas
of convergence. Lower---Magnetic isochrons and prominent faults and
pseudofaults near the Juan Fernandez microplate (JFMP). Brunhes anomaly
is stippled. Diagonal hatching represents compressional ridges or other
complex structures. Figure and caption are modified from
Searle et al. [1993].
Figure 3: Java-Sumatra subduction zone, with tectonic features, earthquake
slip vectors, and plate-motion vectors. Inset shows horizontal earthquake
slip directions (circles), the trench-normal direction (solid line), and
azimuths predicted by the NUVEL-1 Australia-Eurasia angular velocity.
Note how the earthquake slip vectors parallel the trench-normal direction
rather than the predicted convergence direction. Figure is modified from
McCaffrey [1991].