Abstract

SUMMARY The 1992 Nicaragua earthquake was a ‘tsunami earthquake’, which generated tsunamis disproportionately large for its surface wave magnitude Ms = 7.2. Seismological studies and tsunami simulation indicated that the event was a slow earthquake, which occurred on the plate boundary between the subducting Cocos plate and the overriding Caribbean plate. We present a finite element model that enables us to estimate for the first time the temperature and inferred frictional conditions in the rupture area of a tsunami earthquake. Direct and indirect observations are used to constrain all model parameters, and surface heat-flux measurements provide independent information to verify the model results. Furthermore, we used a genetic algorithm to perform a sensitivity analysis of all model parameters and to define the spatial range of thermally defined updip limit of the seismogenic zone. The earthquake nucleated in the seismogenic zone at temperatures of ∼150 ◦ C and propagated updip towards the trench axis. The centroid or centre of mass of moment release was located in a region characterized by temperatures of ∼50 ◦ C. Thus, the rupture propagated through a region where plate motion is normally accommodated by aseismic creep. Our observations support a model in which tsunami earthquakes nucleate in the seismogenic zone near its updip limit. However, in such an environment coupled asperities are perhaps too small to cause large earthquakes. Seamounts, however, are abundant on the incoming Cocos plate. Therefore, in addition to temperature-dependent metamorphic induration of sediments, increased normal stress by seamount subduction may contribute to accumulate stress sufficiently large to release enough energy near the updip limit of the seismogenic zone to promote dynamic slip along a )

Highlights

  • Any great shallow subduction zone earthquake is expected to be followed by a substantial tsunami caused by the large displacement of water near the seafloor

  • In order to cause slip along the shallow normally aseismic basal decollement, tsunami earthquakes may nucleate in the seismogenic zone below the updip limit with enough energy to dynamically propagate updip (Scholz 1998; Seno 2002)

  • We developed a thermal finite element (FE) model to yield the thermal state of the coupling zone and to constrain the thermally defined updip limit of the rupture area

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Summary

INTRODUCTION

Any great shallow subduction zone earthquake is expected to be followed by a substantial tsunami caused by the large displacement of water near the seafloor. Byrne et al (1988) suggested that unconsolidated sediments in the upper part of the subduction thrust cause stable sliding and prevent earthquake nucleation and rupture propagation They postulated that the updip limit of the seismogenic zone occurs at the transition from the sedimentary accretionary prism to the backstop of competent continental rock. In order to cause slip along the shallow normally aseismic basal decollement, tsunami earthquakes may nucleate in the seismogenic zone below the updip limit with enough energy to dynamically propagate updip (Scholz 1998; Seno 2002). New heat-flux data, measured on the continental slope off Nicaragua, provided independent constraints for a genetic algorithm (GA), which we used to find model parameters in agreement with our data and to estimate the uncertainties in the computed thermal state of the rupture zone

T H E 1 9 9 2 NICAR AG UA E A RT H QUA K E
THE NUMERICAL MODEL
Parameter constraints
Initial model
Genetic algorithm
NUMERICAL EXPERIMENTS
DISCUSSION AND CONCLUSIONS
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