The New Madrid seismic zone (NMSZ) in the central United States is the most
seismically active intraplate region in North America. It includes two
SW-NE-trending zones of right-lateral strike-slip faulting on subvertical
faults and a zone of thrust faulting on 30
SW-dipping plane at a left
step-over between the strike-slip fault zones (Figure 30.1). Three
widely felt magnitude
7-8 earthquakes occurred in the
250 km zone
in the the winter of 1811-1812, and the central thrust zone was sufficiently
displaced during the 7 February 1812 event to create a waterfall on the
Mississippi river.
The NMSZ is located within a failed rift that was active about 600 million years ago, followed by period of magmatic reactivation and igneous intrusion of mafic plutons 80 to 60 million ago. These episodes of activity introduced heterogeneities into the crust that may act as stress concentrators for the late Holocene seismicity, possibly initiated by the most recent deglaciation event (Grollimund and Zoback, 2001). Paleoseismic evidence indicates that 1811-1812 sized events have occurred throughout the late Holocene, most recently around 1450 and 900 A.D., but the small cumulative fault offsets inferred from seismic reflection data suggest that the current high level of seismic activity initiated recently, and there is scant paleoseismic evidence for more than 4 episodes prior to the historic events.
Low rates of strain and the lack of apparent active surface tectonics suggest
that the central and eastern U.S. are within the stable interior of the North
America plate. Geodetic studies of broadscale deformation within this region
generally find that relative station velocities are consistent (
mm/yr)
with a rigid plate with strain rates not significantly differing from zero.
High strain rates (
100 nanostrain/yr) were reported within a network
spanning the southern NMSZ based on a 1991 GPS survey and triangulation data
collected in the 1950's (Liu et al., 1992). We present new strain rate
estimates within this southern NMSZ network from GPS surveys conducted in 1993
and 1997 that show the recent deformation rates are not significantly greater
than zero.
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The primary network consists of triangulation benchmarks installed in the mid-1950's that were reoccupied using GPS in 1991 by NGS. Enough of the benchmarks had survived to allow 40-year averaged shear-strain rates to be estimated. This network was reoccupied by GPS in 1993 and 1997 and stations were added to better span the southern seismic zone and the western rift boundary (Figure 30.1).
We processed the data from the 3 GPS surveys using GAMIT/GLOBK software using many of the same techniques used to process the BARD observations (Murray and Segall, 2001). Definition of a self-consistent reference frame is complicated by major changes to the global fiducial network that occurred between the 1991 and 1993 surveys. To better define the velocity frame throughout this period, we included SOPAC global solutions obtained for 45 days, at 64-day intervals, between March 1991 and December 1998. These solutions provide sufficient observations to estimate the positions and velocities of the fiducial stations included in our NMSZ analysis during each interval between significant changes of the station equipment and reference monuments. We defined a North America frame by minimizing the horizontal velocities of 15 stations, which had an rms deviation of 3.5 mm in position and 0.5 mm/yr in velocity.
The velocities of 32 sites in the NMSZ region are well determined with respect
to the North America frame (Figure 30.2). The average horizontal velocity of the 32 stations relative to
North America is
mm/yr at N
E, which significantly differs
from zero (all quoted uncertainties are 95% confidence). The apparent average
northward motion is due primarily to stations located in the interior of the
network, whereas the average motion of the outlying stations (BLUF, HOPE, GP47,
BROA, GP17) is
mm/yr, N
E,
consistent with their being on stable North America.
We estimated strain rates using 1950's triangulation data to compare with the
Liu et al. (1992) results. Because triangulation data are relatively
insensitive to distances and the scale of the network, we estimated engineering
shear strain rates,
and
, from which
the maximum shear-strain rate
and direction of maximum
contraction can be derived. Liu et al. (1992) found that shear-strain
rates in a 22-station network (Figure 30.1) were significantly
greater than zero, particularly in the western half of the network that spans
the rift boundary, with
nanoradian/yr. Using the
same stations, but including GPS data from all 3 years, we find the estimated
shear strain rates in all cases do not significantly differ from zero. For
example,
using all or just the western stations is
or
nanoradian/yr, respectively. Therefore, in contrast to the
1992 study, we find no evidence for high strain rates in the southern New
Madrid seismic zone.
The average motion of the interior stations relative to the outlying stations
is
mm/yr, N
E, with the most central stations tending to
have velocities slightly elevated above this level. The spatial coherence of
this pattern suggests that some deformation--albeit marginally
significant--may be present in the region. Projecting the average motion onto
the N
E seismic trend yields 0.7 parallel and -0.6 mm/yr perpendicular
components, which is opposite of that predicted by simple elastic strain
dislocation models that assume zero far-field deformation and backslip on the
faults defined by seismic and paleoseismic studies. We are currently
investigating alternative explanations for this tantalizing signal, such as
from a gravitational instability of the underlying rift pillow (Pollitz et
al., 2002), or from the relaxation of a weakened lower crustal zone proposed
by Kenner and Segall (2000). This latter model, which predicts low rates
of strain consistent with our geodetic observations, shows that low strain
rates do not necessarily preclude the possibility of repeating large intraplate
earthquakes, and that the seismic hazards in the NMSZ are still likely to be
high.
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We appreciate previous support for this project by the NSF. We thank Stacy Kerkela, Stephanie Prejean, and the staff and students of CERI in Memphis, Tennessee for assistance conducting the 1997 survey.
Grollimund, B., and M. D. Zoback, Did deglaciation trigger intraplate seismicity in the New Madrid seismic zone?, Geology, 29, 175-178, 2001.
Kenner, S. J., and P. Segall, A mechanical model for intraplate earthquakes: Application to the New Madrid seismic zone, Science, 289, 2329-2332, 2000.
Liu, L. B., M. D. Zoback, and P. Segall, Rapid intraplate strain accumulation in the New Madrid seismic zone, Science, 257, 1666-1669, 1992.
Murray, M. H., and P. Segall, Modeling broadscale deformation in northern California and Nevada from plate motions and elastic strain accumulation, Geophys. Res. Lett., 28, 4315-4318, 2001.
Pollitz, F. F., L. Kellogg, and R. Bürgmann, Sinking mafic body in a reactivated lower crust: A mechanism for stress concentration in the New Madrid Seismic Zone, Bull. Seismol. Soc. Am., 91, 1882-1897, 2002.
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