近130 ka以来地球磁场相对强度变化:南海南部NS93-5钻孔记录     

杨小强  张贻男  高芳蕾  周文娟  周永章 《热带地理》2006,26(1):1-5,17

选择位于南沙台地的NS93-5钻孔进行地磁场相对强度的研究.根据氧同位素地层学(MIS1～MIS5),建立130 ka以来的沉积序列.岩石磁场研究表明,沉积物中的磁性矿物主要为1～15μm的细粒磁铁矿,磁性矿物浓度的变化在同一数量级之内,而且沉积物磁性比较稳定.选择NRM/x作为相对磁场强度的估计指标,发现在10～100ka时间尺度上,可以很好地进行全球对比,千年时间尺度上尽管有一定的误差,但也可以进行有效对比.130ka以来,有4次强度变化的低谷,分别发生在32.5～40 ka、44～52.5 ka、6  相似文献   

Crustal structure of a super-slow spreading centre:a seismic refraction study of Mohns Ridge, 72° N     

F. Klingelhöfer  L. Géli  L. Matias  N. Steinsland  & J. Mohr 《Geophysical Journal International》2000,141(2):509-526

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Canadian expedition to study the Alpha Ridge complex: results of the seismic refraction survey     

I. Asudeh  A. G. Green  D. A. Forsyth 《Geophysical Journal International》1988,92(2):283-301

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How partial melts of mafic lower crust affect ascending magmas at oceanic ridges     

Astri J. S. Kvassnes  Timothy L. Grove 《Contributions to Mineralogy and Petrology》2008,156(1):49-71

We present experiments showing that the lower oceanic crust should melt efficiently and quickly when heated by hot ascending magmas. Average plagioclase–olivine and plagioclase–augite pairs from the lower crust at the Southwest Indian Ridge have melt–mineral saturation boundaries at 1,190 and 1,154°C, respectively, and melt rapidly (>0.01 mm/h) at 50°C or more above these temperatures. Melting experiments performed on olivine–plagioclase and augite–plagioclase mineral pairs from actual oceanic lower crustal rock samples and under conditions applicable to a MOR setting (1,220–1,330°C, 1 atm, quartz–fayalite–magnetite oxygen buffer, 0.25–24 h) indicate that the resulting disequilibrium melts are linear mixes of the mineral compositions. The rates of melting are slower than the rate of heat-diffusion into a sample and are approximated as: Our results indicate that great care must be taken in backward models using basalt chemistry alone to explore mantle-melting processes, assuming only crystallization and fractionation during ascent, as partial melts may mix with intruded hot magma.  相似文献   

Results of a sea-floor electromagnetic survey over a sedimented hydrothermal area on the Juan de Fuca Ridge     

D. C. Nobes  L. K. Law  R. N. Edwards 《Geophysical Journal International》1992,110(2):333-346

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选取岭参数的一个新方法   总被引：2，自引：1，他引：1  

归庆明 《测绘工程》1997,6(1):14-19

当法方程的系数阵呈病态时,平差参数的最小二乘估计不再是一个良好好估计。为改进最小二乘估计,许多学者提出众多的有偏估计方法,其中影响最大的是岭估计和主要估计。  相似文献   

Excursion to kettering and thrapston: Saturday,July 7th, 1900     

J.F. Blake 《Proceedings of the Geologists' Association. Geologists' Association》1900,16(10):516-517

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Bathymetry of the Reykjanes Ridge     

Keeton  J. A.  Searle  R. C.  Peirce  C.  Parsons  B.  White  R. S.  Sinha  M. C.  Murton  B. J.  Parson  L. M. 《Marine Geophysical Researches》1997,19(1):55-64

We present a series of 1:200,000 scale maps of the bathymetry of the Reykjanes Ridge. The data are divided into four maps, extending 630 km along the ridge axis and between 30 and 100 km off-axis. This compilation of bathymetry data is extremely detailed, gridded at approximately 100 m resolution, and with almost no gaps. The Reykjanes Ridge is one of the best examples of a hotspot-dominated ridge, whose characteristics are influenced by its proximity to the Iceland plume. Many fundamental questions may be addressed at the Reykjanes Ridge, which is why the BRIDGE programme identified it as one of its four regional projects. These maps represent a BRIDGE contribution to the general scientific community.  相似文献   

Structural analysis of the segmentation of the Central Indian Ridge between 20°30′S and 25°30′S (Rodriguez Triple Junction)     

Anne Briais 《Marine Geophysical Researches》1995,17(5):431-467

The morphological characteristics of the segmentation of the Central Indian Ridge (CIR) from the Indian Ocean Triple Junction (25°30S) to the Egeria Transform Fault system (20°30S) are analyzed. The compilation of Sea Beam data from R/VSonne cruises SO43 and SO52, and R/VCharcot cruises Rodriguez 1 and 2 provides an almost continuous bathymetric coverage of a 450-km-long section of the ridge axis. The bathymetric data are combined with a GLORIA side-scan sonar swath to visualize the fabric of the ridge and complement the coverage in some areas. This section of the CIR has a full spreading rate of about 50 mm yr^–1, increasing slightly from north to south. The morphology of the CIR is generally similar to that of a slow-spreading center, despite an intermediate spreading rate at these latitudes. The axis is marked by an axial valley 5–35 km wide and 500–1800 m deep, sometimes exhibiting a 100–600 m-high neovolcanic ridge. It is offset by only one 40km offset transform fault (at 22°40S), and by nine second-order discontinuities, with offsets varying from 4 to 21 km, separating segments 28 to 85 km long. The bathymetry analysis and an empirical orthogonal function analysis performed on across-axis profiles reveal morphologic variations in the axis and the second-order discontinuities. The ridge axis deepens and the relief across the axial valley increases from north to south. The discontinuities observed south of 22°S all have morphologies similar to those of the slow-spreading Mid-Atlantic Ridge. North of 22°S, two discontinuities have map geometries that have not been observed previously on slow-spreading ridges. The axial valleys overlap, and their tips curve toward the adjacent segment. The overlap distance is 2 to 4 times greater than the offset. Based on these characteristics, these discontinuities resemble overlapping spreading centers (OSCs) described on the fast-spreading EPR. The evolution of one such discontinuity appears to decapitate a nearby segment, as observed for the evolution of some OSCs on the EPR. These morphological variations of the CIR axis may be explained by an increase in the crustal thickness in the north of the study area relative to the Triple Junction area. Variations in crustal thickness could be related to a broad bathymetric anomaly centered at 19°S, 65°E, which probably reflects the effect of the nearby Réunion hotspot, or an anomaly in the composition of the mantle beneath the ridge near 19°S. Other explanations for the morphological variations include the termination of the CIR at the Rodriguez Triple Junction or the kinematic evolution of the triple junction and its resultant lengthening of the CIR. These latter effects are more likely to account for the axial morphology near the Triple Junction than for the long-wavelength morphological variation.  相似文献   

Second-order ridge axis discontinuities in the south Atlantic: Morphology,structure, and evolution   总被引：1，自引：0，他引：1  

N. R. Grindlay  P. J. Fox  K. C. MacDonald 《Marine Geophysical Researches》1991,13(1):21-49

Continuous along-axis Sea Beam coverage of the slow-intermediate spreading (34–38 mm yr⁻¹ full rate) southern Mid-Atlantic Ridge (25°–27°30′S and 31°–38° S) shows that the ridge axis is segmented by both rigid and non-rigid discontinuities. Following the model of Macdonald et al. (1988b), a hierarchy of four orders is proposed for ridge axis discontinuities based on a continuum of relative age and distance offset across the discontinuites. This paper discusses the characteristics associated with five second-order discontinuities found in the areas surveyed. First-order discontinuities represent rigid offsets, transform faults, whereas non-rigid discontinuities fall into the second, third and fourth orders. Like transform fault boundaries, second-order discontinuities have distinctive morphologic signatures both on and off-axis-discordant zones — and therefore are better defined than third- or fourth-order discontinuities. Second-order discontinuities are offsets that range in distance from less than 10 km to approximately 30 km and vary in age offset from 0.5 to approximately 2.0 m.y. The variable morphotectonic geometries associated with these discontinuities indicate that horizontal shear strains are accommodated by both extensional and strike-slip tectonism and that the geometries are unstable in time. Three characteristic geometries are recognized: (1)en echelon jog in the plate boundary where ridge axis tips overlap slightly, (2)en echelon jog in the plate boundary where ridge axes are separated by an extensional basin whose long axis is oriented parallel to the strike of the adjoining ridge axes, and (3) oblique offset characterized by a large extensional basin that is oriented approximately 45° to the strike of the ridge axes. In the case of the third type, evidence for short strands of strike-slip tectonism that link an obliquely oriented extensional basin flanking ridge tips is often apparent. Analysis of the detailed bathymetric and magnetic data collected over the second-order discontinuities and their off axis terrain out to 5–7 m.y. documents that second-order discontinuities can follow several evolutionary paths: they can evolve from transform fault boundaries through prolonged asymmetric spreading, they may migrate along strike leaving a V-shaped wake, and they may remain in approximately the same position but oscillate slightly back and forth. In addition, a small change in the pole of relative motion occurring 4–5 Ma is thought to have resulted in the initiation of at least one second-order discontinuity in the survey area. A geologic model is proposed which involves the interplay of lithospheric thickness, asymmetric spreading, temporal and spatial variability of along-axis magmatic input and changes in the poles of relative motion to explain the origin, morphology and evolution of second-order ridge axis discontinuities.  相似文献