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Simple analytic model for subduction zone thermal structure 总被引：4，自引：0，他引：4
J. Huw Davies 《Geophysical Journal International》1999,139(3):823-828
A new analytic model is presented for the thermal structure of subduction zones. It applies to the deeper regions of a subduction zone, where the overriding mantle is no longer rigid but flows parallel to the slab surface. The model captures the development of one thermal boundary layer out into the mantle wedge, and another into the subducting slab. By combining this model with the analytic model of Royden (1993a , b ), which applies to regions in which the overriding plate is rigid, a nearly complete analytic model for the thermal structure of a steady-state subduction zone can be achieved. A good agreement is demonstrated between the output of the combined analytic model and a numerical finite element calculation. The advantages of this analytic approach include (1) efficiency (only limited computing resources are needed); (2) flexibility (non-linear slab shape, and processes such as erosion, and shear heating are easily incorporated); and (3) transparency (the effect of changes in input variables can be seen directly). 相似文献
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Flexure of subducted slabs 总被引：2，自引：0，他引：2
The subducted lithosphere is regarded as a thin elastic plate that bends as a consequence of slab pull, the pressure of the asthenospheric flow induced by the subduction motion and the pressure exerted by the asthenospheric motion relative to the lithosphere. In westward subductions the latter factor enhances the slab pull, but in eastward subductions it opposes it. As a result, the subduction angle changes continuously with depth, following an elastic profile: it is smaller in eastward subductions and larger in those having a westward direction. The application of the model to 13 subducted slabs shows a good fit between the observed and the calculated shapes of the slabs. 相似文献
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Numerical comparison of different convergent plate contacts: subduction channel and subduction fault 总被引：2，自引：0，他引：2
At convergent plate boundaries, the properties of the actual plate contact are important for the overall dynamics. Convergent plate boundaries both mechanically decouple and link tectonic plates and accommodate large amounts of strain. We investigate two fundamental physical states of the subduction contact: one based on a fault and the other based on a subduction channel. Using a finite element method, we determine the specific signatures of both states of the subduction contact. We pay particular attention to the overriding plate. In a tectonic setting of converging plates, where the subducting plate is freely moving, the subduction channel reduces compression relative to the fault model. In a land-locked basin setting, where the relative motion between the far field of the plates is zero, the subduction channel model produces tensile stress regime in the overriding plate, even though the amount of slab roll-back is small. The fault model shows a stronger development of slab roll-back and a compressive stress regime in the upper plate. Based on a consistent comparison of fault and channel numerical models, we find that the nature of the plate contact is one of the controlling factors in developing or not of backarc extension. We conclude that, the type of plate contact plays a decisive role in controlling the backarc state of stress. To obtain backarc extension, roll-back is required as an underling geodynamic process, but it is not always a sufficient condition. 相似文献
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ScS wave splitting of deep earthquakes around Japan 总被引：4，自引：0，他引：4
Yoshihiro Hiramatsu Masataka Ando Yuzo Ishikawa 《Geophysical Journal International》1997,128(2):409-424
ScS wave splitting of five deep earthquakes in subduction zones near Japan is investigated using horizontal seismograms recorded al JMA stations. For each earthquake, we clearly observe uniform ScS wave splitting in all stations over Japan, especially for the events located south of Honshu in 1982, 1984 and 1993. However, the directions of fast-polarized waves of these events differed by a maximum of about 50° from one another. The orientation of fast-polarized waves in the 1982 event was NNW-SSE; those in the two later events WNW-ESE. We also recognize this discrepancy in the results of the analysis of the 1971 Sea of Okhotsk event reported by Fukao (1984). The Sakhalin Islands event in 1990 reveals a linear particle motion without such a change in direction of the second arrivals, implying no anisotropy. These observations are interpreted as indicating an anisotropic region within the slab near the earthquake sources but not beneath the receivers, since the orientations of fast-polarized waves recorded at each station are not common to all the earthquakes. Furthermore, we consider that anisotropy exists non-uniformly within the slab. The event in 1982, which occurred in almost the same area as those in 1984 and 1993, showed a fast direction different from the events in 1984 and 1993. The 1982 event was 179 km deep, but the two later events were at 398 km and 360 km, respectively. The fast direction observed from the 1982 event is parallel to the fossil plate motion, whereas those from the events in 1984 and 1993 are parallel to the compression axis within the subducting slab. The depth of 400 km is a phase boundary, where olivine changes to β spinel. We consider that the most likely cause of the change in anisotropy direction is the re-orientation of crystals associated with the phase change of olivine to β spinel due to subduction of the slab. 相似文献
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Seismic phase conversions provide important constraints on the layered nature of subduction zone structures. Recordings from digital stations in North Island, New Zealand, have been examined for converted ScS ‐to‐ p ( ScSp ) arrivals from deep (>150 km) Tonga–Kermadec earthquakes to image layering in the underlying Hikurangi subduction zone. Consistent P ‐wave energy prior to ScS has been identified from stations in eastern and southern North Island, where the subducted plate interface is at a depth of between 15 and 30 km. Two ScS precursors are observed. Ray tracing indicates that the initial precursor ( ScSp 1 ) corresponds to conversion from the base of an 11–14 km thick subducting Pacific crust. The second precursor is interpreted as a conversion from the top of the subducting plate. The amplitude ratio, ScSp 1 : ScS , increases from 0.10 to 0.19 from northern to southern North Island. This is within the range expected from a simple first‐order velocity discontinuity at an oceanic Moho. A 1–2 km thick layer of low‐velocity sediment at the top of the subducting plate is required to explain the remaining ScSp waveform. Our results imply that the abnormally thick Hikurangi–Chatham Plateau has been subducting beneath New Zealand for at least 2.9 Myr, thus explaining the high uplift rates observed across eastern North Island. 相似文献
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The migration of teleseismic receiver functions yields high-resolution images of the crustal structure of western Crete. Data were collected during two field campaigns in 1996 and 1997 by networks of six and 47 short-period three-component seismic stations, respectively. A total of 1288 seismograms from 97 teleseismic events were restituted to true ground displacement within a period range from 0.5 to 7 s. The application of a noise-adaptive deconvolution filter and a new polarization analysis technique helped to overcome problems with local coda and noise conditions. The computation and migration of receiver functions results in images of local crustal structures with unprecedented spatial resolution for this region. The crust under Crete consists of a continental top layer of 15–20 km thickness above a 20–30 km thick subducted fossil accretionary wedge with a characteristic en echelon fault sequence. The downgoing oceanic Moho lies at a depth of 40–60 km and shows a topography or undulation with an amplitude of several kilometres. As a consequence of slab depth and distribution of local seismicity, the Mediterranean Ridge is interpreted as the recent accretionary wedge. 相似文献
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J. Martinod F. Funiciello C. Faccenna S. Labanieh V. Regard 《Geophysical Journal International》2005,163(3):1137-1150
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Summary. Five major convergent plate boundaries (South America, Izu–Bonin–Marianas, New Hebrides, Tonga–Kermadec and Indonesia) show strong variations in levels of background seismicity on scales ranging from tens to thousands of kilometres. These variations were tested using two statistical approaches and we conclude that small earthquakes are not distributed randomly along these zones.
Two types of large-scale seismicity variations (termed first order) were recognized. First, regions with dimensions on the order of 100 km with extremely high seismicity levels (first-order actives). One such region was recognized in each of the zones studied. Second, large-scale (500 to several thousand kilometres) differences in the level of background seismicity along a given plate boundary. Regions with consistent levels of background seismicity are termed first-order segments.
We examined each first-order segment for smaller scale variations. Ten regions ranging in length from 40 to 170 km with anomalously high seismicity levels were recognized. Fifty-three regions ranging in length from 25 to 355 km were found to have anomalously low seismicity levels. Thus, areas with anomalously high levels of activity are rare in subduction zones.
These observations indicate that background seismicity in subduction zones is not randomly distributed along the strike of the zones. It seems likely that the observed variations reflect tectonic differences. In fact, many of the seismicity variations which we observed appear to be spatially related to features on the seafloor or on the overriding plate. If this is so, then they may provide a powerful tool for characterizing subduction zones and understanding the mechanisms of earthquake generation. 相似文献
Two types of large-scale seismicity variations (termed first order) were recognized. First, regions with dimensions on the order of 100 km with extremely high seismicity levels (first-order actives). One such region was recognized in each of the zones studied. Second, large-scale (500 to several thousand kilometres) differences in the level of background seismicity along a given plate boundary. Regions with consistent levels of background seismicity are termed first-order segments.
We examined each first-order segment for smaller scale variations. Ten regions ranging in length from 40 to 170 km with anomalously high seismicity levels were recognized. Fifty-three regions ranging in length from 25 to 355 km were found to have anomalously low seismicity levels. Thus, areas with anomalously high levels of activity are rare in subduction zones.
These observations indicate that background seismicity in subduction zones is not randomly distributed along the strike of the zones. It seems likely that the observed variations reflect tectonic differences. In fact, many of the seismicity variations which we observed appear to be spatially related to features on the seafloor or on the overriding plate. If this is so, then they may provide a powerful tool for characterizing subduction zones and understanding the mechanisms of earthquake generation. 相似文献
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