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41.
The Longmenshan fault, which defines the eastern edge of the Tibetan Plateau, is one of the steepest margins of the plateau with a sharp elevation drop of about 4 km over a distance less than 100 km across the Longmenshan fault. The mechanism which is responsible for controlling and maintaining the elevation difference is highly debated. Using multiple observations including seismic velocity model, Moho depth, effective elastic thickness of the lithosphere, we conducted a quantitative study for elucidating the contributions from crust and lithospheric mantle by an integrated analysis of lithospheric isostasy and flexure. It is shown that the topography of the Longmenshan fault is supported by both lithospheric isostasy and flexure statically, and lower crustal channel flow and mantle convection dynamically. Different mechanisms have different weights for contribution to the topography of the Songpan-Ganzi block and the Sichuan Basin. The static and dynamic support contribute roughly the same to the topographic difference of ~4 km between the two sides of the Longmenshan fault. The static topographic difference of ~2 km is mainly resulted from the lithospheric isostasy, while the dynamic one of ~2 km is contributed by the uprising of the accumulated material in the lower crust beneath the Songpan-Ganzi block and the downward drag force caused by the upper mantle convection under the Sichuan Basin. It is thus suggested that the lower crustal flow and upper mantle convection are dynamic forces which should be taken into account in the studies on the dynamics in the Longmenshan and surrounding regions. 相似文献
42.
A. B. Watts D. P. McKenzie B. E. Parsons M. Roufosse 《Geophysical Journal International》1985,83(1):263-298
Summary. Surface-ship and satellite derived data have been compiled in new free-air gravity anomaly, bathymetry and geoid anomaly maps of the Pacific Ocean basin and its margin. The maps are based on smoothed values of the gravity anomaly, bathymetry and geoid interpolated on to a 90 × 90 km grid. Each smoothed value was obtained by Gaussian filtering measurements along individual ship and subsatellite tracks. The resulting maps resolve features in the gravity, bathymetry and geoid with wavelengths that range from a few hundred to a few thousand kilometres. The smoothed values of bathymetry and geoid anomaly have been corrected for age. The resulting maps show the Pacific ocean basin is associated with a number of ENE–WSW-trending geoid anomaly highs with amplitudes of about ± 5 m and wavelengths of about 3000 km. The most prominent of these highs correlate with the Magellan seamounts–Marshall Gilbert Islands–Magellan rise and the Hess rise–Hawaiian ridge regions. The correlation between geoid anomaly and bathymetry cannot be explained by models of static compensation, but is consistent with a model in which the geoid anomaly and bathymetry are supported by some form of dynamic compensation. We suggest that the dynamic compensation, which characterizes oceanic lithosphere older than 80 Myr, is the result of mantle convection on scales that are smaller than the lithospheric plates themselves. 相似文献
43.
44.
《The Australian geographer》1991,22(2):178-184
Significant elements of the Australian landscape date from Mesozoic or earlier times. Australia did not separate completely from other Gondwanan components until Early Tertiary times and these Mesozoic and older elements can therefore be regarded as Gondwanan. During the separation and northern drift of the continent and particularly in Late Jurassic and earlier Cretaceous times the sea invaded and spread across much of the erstwhile landmass. The associated sediments not only covered and preserved much of the pre‐existing land surface, but they also augmented the effects of thalassostatic loading of the basins, causing further subsidence. Hinge lines developed near the coastal zones of the times, so that subsidence of the basins caused adjacent land masses to rise. Many old land surfaces have been re‐exposed at the former oceanic margins, but epigene forms are preserved high in the relief on the uplifted blocks. They survive partly because, as Crickmay (1976) suggested, rivers effectively erode at and near their channels; the divides remain untouched. A reinforcement effect also operates because the valleys are wet sites, the interfluves dry. Hence weathering and erosion proceed apace in the former while the latter are stable, allowing palaeoforms to survive. 相似文献
45.
The present-day basement depth of the seafloor in the absence of sediment loading was inferred along a traverse crossing the
Southern Tyrrhenian Basin. A correction for sediment loading was proposed on the basis of density, seismic velocity and porosity
data from selected deep boreholes. The empirical relation between sediment correction and seismic two-way travel time was
extrapolated downward by applying the Nafe–Drake curve and a specific porosity–depth relation. The sediment loading response
of the basement calculated for flexural isostasy is on average about one hundred meters lower than results for local isostasy.
A pure lithosphere extensional model was then used to predict quantitatively the basement subsidence pattern on the margins
of the basin. The basement depth is consistent with uniform extension model predictions only in some parts of the margins.
The observed variability in the region of greatest thinning (transition from continental to oceanic crust) is attributable
to the weakening effect caused by diffuse igneous intrusions. Subsidence of the volcanic Calabrian–Sicilian margin is partly
accounted for by magmatic underplating. The comparison of the calculated subsidence with an oceanic lithosphere cooling model
shows that subsidence is variable in some areas, particularly in the Marsili Basin. This argues for a typical back-arc origin
for the Tyrrhenian Basin, as a result of subduction processes. By taking into account the geodynamic setting, stratigraphic
data from the deepest hole and the terrestrial heat flow, we reconstructed the paleotemperatures of cover sediments. The results
suggest that low temperatures generally have prevailed during sediment deposition and that the degree of maturation is expected
not to be sufficient for oil generation processes. 相似文献
46.
47.
地壳均衡是地球科学的一个基本概念,其理论基础为“轻地壳(密度较小)漂浮在重地幔(较稠密)之上”。均衡理论(如冲压假说、弹性板理论等)和模型(如Airy模型、Pratt模型及弹性板模型等)的产生及发展对研究岩石圈流变学性质、圈层相互作用及造山作用等地球动力学过程有着重要意义。本文总结了相关均衡理论、模型及计算方法,并结合其在不同空间尺度构造地貌现象研究中的运用,包括:① 冰川均衡调整研究中不同模型的优化及其对全球海平面变化的指示意义、② 阐明海山洋岛发育过程及其制约因素、③ 利用弹性板模型重建山脉隆升和盆地挠曲沉降史并进一步探讨二者之间的相互作用、④ 通过研究变形湖滨线有效地约束地球的相关物理参数、⑤ 建立河流三角洲发育特征模型并服务于现代社会经济、⑥ 揭示水库蓄水导致的地壳挠曲变形与浅部地质灾害发育的关系及 ⑦ 同震滑坡对局部地貌改造的影响,讨论并展望了未来地壳均衡在构造地貌学领域的发展方向,即结合高精度大地测量技术与地质年代学方法,定量地解决构造地貌研究中的关键问题,更全面、系统地了解地表过程、地球深部过程与动力学和地球圈层之间的相互作用。 相似文献
48.
Most of the East European Craton lacks surface relief; however, the amplitude of topography at the top of the basement exceeds 20 km, the amplitude of topography undulations at the crustal base reaches almost 30 km with an amazing amplitude of ca. 50 km in variation in the thickness of the crystalline crust, and the amplitude of topography variations at the lithosphere–asthenosphere boundary exceeds 200 km. This paper examines the relative contributions of the crust, the subcrustal lithosphere, and the dynamic support of the sublithospheric mantle to maintain surface topography, using regional seismic data on the structure of the crystalline crust and the sedimentary cover, and thermal and large-scale P- and S-wave seismic tomography data on the structure of the lithospheric mantle. For the Precambrian lithosphere, an analysis of Vp/Vs ratio at 100, 150, 200, and 250 km depths does not show any age-dependence, suggesting that while Vp/Vs ratio can be effectively used to outline the cratonic margins, it is not sensitive to compositional variations within the cratonic lithosphere.Statistical analysis of age-dependence of velocity, density, and thermal structure of the continental crust and subcrustal lithosphere in the study area (0–62E, 45–72N) allows to link lithospheric structure with the tectonic evolution of the region since the Archean. Crustal thickness decreases systematically with age from 42–44 km in regions older than 1.6 Ga to 37–40 km in the Paleozoic–Mesoproterozoic structures, and to ca. 31 km in the Meso-Cenozoic regions. However, the isostatic contribution of the crust to the surface topography of the East European Craton is almost independent of age (ca. 4.5 km) due to an interplay of age-dependent crustal and sedimentary thicknesses and lithospheric temperatures.On the contrary, the contribution of the subcrustal lithosphere to the surface topography strongly depends on the age, being slightly positive (+ 0.3 + 0.7 km) for the regions older than 1.6 Ga and negative (− 0.5–1 km) for younger structures. This leads to age-dependent variations in the residual topography, i.e. the topography which cannot be explained by the assumed thermal and density structure of the lithosphere, and which can (at least partly) originate from the dynamic component caused by the mantle flow. Positive dynamic topography at the cratonic margins, which exceeds 2 km in the Norwegian Caledonides and in the Urals, clearly links their on-going uplift with deep mantle processes. Negative residual topography beneath the Archean-Paleoproterozoic cratons (− 1–2 km) indicates either a smaller density deficit (ca. 0.9%) in their subcrustal lithosphere than predicted by global petrologic data on mantle-derived xenoliths or the presence of a strong convective downwelling in the mantle. Such mantle downflows can effectively divert heat from the lithospheric base, leading to a long-term survival of the Archean-Paleoproterozoic lithosphere. 相似文献
49.
50.
Detlef Wolf 《Geophysical Journal International》1996,127(3):801-805
For more than 30 years, Sauramo's (1958) shoreline diagram of the Fennoscandian uplift has been used in geophysical studies for estimates of the glacial-isostatic decay spectrum in order to infer from it the viscosity stratification in the Earth's mantle below Fennoscandia. The intent of the present note is to point out that more recent geological studies suggest that Sauramo's shoreline diagram is an incorrect representation of the Fennoscandian uplift. Geophysical interpretations based on the diagram may therefore require revision. 相似文献