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131.
地表风蚀物理过程风洞实验的初步研究   总被引:13,自引:5,他引:13  
本文介绍了研究地表风蚀物理过程中风洞实验的方法、内容及结果。实验表明:净风对土表的风蚀作用微弱,即使在遭到大风吹刮时,土表的结壳仍不易受到破坏。但在挟沙气流作用下,却能使土表结壳遭到破坏,风蚀发展异常迅速。自然形成的土表结壳、经风选被粗化的土表和长有草丛的地表均有抑制风蚀的保护作用。本实验在方法上虽属初步尝试,但能说明沙漠化物理过程的一般机制,并为防治按漠化的措施提供依据。  相似文献   
132.
利用DDA(Discrete Dipole Approximation)算法产生的旋转扁椭球水滴散射特征数据进行了多项式拟合,以3.2mm波长为例,给出了两种偏振状态下后向散射和衰减效率的快速算式。对比分析了快速算式结果和DDA数据的独立样本,结果表明,快算结果的绝对相对误差在5%以内,而耗时仅用DDA算法产生这些数据所用时间的10-6量级。所得结果可直接用于云降水区含扁椭球形水滴情况下的雷达回波模拟、雷达资料定量处理和毫米波雷达的衰减订正等,此方法还可用于其他波长、形状的水滴和冰晶。  相似文献   
133.
构造-沉积分异是地球表层的常见地质现象,发生于沉积盆地、造山带与克拉通等岩石圈构造单元,表现为岩石圈的深、中、浅层始终发生着沉积物、流体、能量与力的交换与分异过程。文中从物质组成、时空分布与力学机制等方面阐述构造-沉积分异的基本特征,并以中国沉积盆地为例进行分析。作者首先将构造-沉积分异定义为“由构造应力、热力、重力、地幔动力等因素引起地表地形差异,从而导致沉积物源、搬运体系与沉积作用变化的过程”;认为构造-沉积分异发生在不同尺度的洋-陆系统、盆-山系统、隆-坳系统、凸-凹系统与高-低地貌系统,受基底结构、强度与活动性的明显控制,构造应力、重力、热力、地幔动力等控制了该分异机制; 强调随时间演变出现构造-沉积分异演化旋回,表现为伸展期裂陷向聚敛期隆坳转变,碳酸盐岩分异台地向统一台地转变。上述控制因素与机制在时空上可以发生复合,导致多类构造-沉积分异作用出现。研究构造-沉积分异作用,可以为重建地球历史、加快矿产资源勘查和改善人类宜居环境做出贡献。  相似文献   
134.
肖斌  刘树根  冉波  杨迪  韩雨樾 《地质论评》2019,65(6):1316-1330
基于金属元素Mn、Co、Cd、Mo的海洋富有机质沉积岩沉积环境和有机质富集主控因素判别指标Al—Co·Mn和Co·Mn—Cd/Mo,能够有效地区分促进有机碳埋藏的两种海洋端元沉积环境:大陆边缘开放/上升洋流环境和滞留的边缘海盆环境。利用这种方法研究了四川盆地北缘城口县月亮坪剖面五峰组和龙马溪组页岩沉积时期的水体环境和有机质富集的主控因素。研究表明五峰组Mn、Co富集程度低,Mo富集程度自下而上明显增大;龙马溪组Mn整体亏损,Co富集程度低,Mo富集程度自下而上明显减小。Al—Co·Mn方法的使用发现滞留环境主要出现在五峰组早期和龙马溪组晚期,以及观音桥段附近,而五峰组中晚期和龙马溪组早—中期水体主要处于开放/上升洋流区。剖面[w(Co)/(μg/g)]·[w(Mn)/(%)]值均小于平均页岩值1.615;五峰组Cd/Mo值整体大于正常海水值0.006,全部小于平均页岩值0.308,龙马溪组整体小于正常海水值。Co·Mn—Cd/Mo联合图版的使用发现月亮坪剖面五峰组和龙马溪组有机质富集主要受到保存条件控制,与使用U/Th、V/Cr、P/Ti、Ba/Al与TOC相关性分析得出的结论一致。基于金属元素Mn、Co、Cd、Mo的判别指标对于判断古生代大陆边缘地区富有机质页岩沉积环境及有机质富集主控因素有较好的效果。  相似文献   
135.
This study addresses the influence of landslide dams on surface water drainage and groundwater flow. In the study area of Scanno Lake and Sagittario River (Central Italy), a limestone rockslide‐avalanche formed a lake, which has an outlet that is occasionally active, showing infiltration into the rockslide dam. Several springs are present at the lake's base and are partly fed by seepage through the rockslide debris. Piezometric surveys, discharge measurements, pumping tests and chemical analyses are tools used to build a conceptual model of the groundwater flow and to evaluate the flow through the rockslide debris. Seasonal water isotopic signatures validate the assumed model, showing a mixing of infiltration recharge and groundwater seepage throughout the rockslide debris. Various recharge areas have been found for springs, pointing out those directly fed by the rockslide debris aquifer. Hypotheses about seasonal groundwater mixing between the regional carbonate aquifer and the rockslide debris aquifer are supported by isotope results. Seasonal changes in groundwater table level due to recharge and surface losses from seasonal outlet have been correlated with isotopic groundwater composition from the rockslide debris aquifer and the downstream springs; this relationship highlights the role of the rockslide dam body on the hydrodynamics of the studied area. Relationships between surface waters and groundwater in the area have been completely understood on the basis of water isotopic fingerprinting, finally obtaining a complete evaluation of groundwater renewable resources and its regimen. Copyright © 2010 John Wiley & Sons, Ltd.  相似文献   
136.
本文以模糊子集论为指导,在迪戴的DCM法的基础上提出了动态聚类-模糊模式识别方法。实际上,它是一种新的模糊聚类的方法。该方法以DCM法的动态聚类部分做为原始数据变换的手段,而将迪戴的强模式概念推广为模糊模式,将强模式识别推广为模糊模式识别。此外,还提出了模糊模式间联系度的概念,从而解决了类间联系、类内典型个体、类间过渡个体、个体对各类的隶属程度以及内部有某种演化趋势的类别的划分等问题。文章还给出了该方法的数学模型和算法概要。最后,通过一个在地质学中的应用实例,说明了该方法的应用效果。  相似文献   
137.
Six years after the 1991 Mt. Pinatubo eruption, deep erosion incisions into the pyroclastic deposits accumulated around the volcano enabled us to investigate the stratigraphy of the climactic deposits both in valley bottoms and on contiguous ridges. Stratigraphic relationships between fall, flow, and surge deposits in the Marella drainage system indicate that during the climactic eruption a progressive shift occurred from an early convective regime, to a transitional regime feeding both the plinian convective column and mostly dilute density currents, to a fully collapsing regime producing mostly dense pyroclastic flows. Syn-plinian dilute density currents (surges) propagated up to ~10 km from the crater, both along valley bottoms and on contiguous ridges of the Marella Valley, whereas post-plinian pyroclastic flows had greater runout (~13 km), were confined to valleys and were not associated with significant surges. Stratigraphic study and grain-size analyses allow the identification of three types of intra-plinian deposits: (a) lower and often coarse-grained surge deposits, emplaced during the accumulation of the coarsest portion of the fallout bed at time intervals of ~16-24 min; (b) upper fine-grained surge deposits, interstratified with the fine-grained portion of the fall bed and emplaced at shorter time intervals of ~3-13 min; and (c) small-volume, channel-confined, massive pumiceous flow deposits interbedded with the upper surges in the upper fine-grained fall bed. Maximum clast size isopleths of 1.6 and 0.8 cm for lithics (ML) and 2.0 and 4.0 cm for pumices (MP) show almost symmetrical distribution around the vent, indicating that the passing of the typhoon Yunya during the climactic eruption had little effect on trajectories of high-Reynold-number clasts. Significant distortion was, however, observed for the 3.2-cm ML and 6.0-cm MP proximal isopleths, whose patterns were probably influenced by the interaction of the clasts falling from column margins with the uprising co-ignimbrite ash plumes. Application of the Carey and Sparks (1986) model to the undisturbed isopleths generated by the umbrella cloud yields a maximum column height of ~42 km, in good agreement with satellite measurements. Systematic stratigraphic and vertical grain-size studies of the plinian fall deposit in the Marella Valley, combined with satellite data and eyewitness accounts, reveal that the carrying capacity of the convective column and related fallout activity peaked in the early phase of the eruption, beginning slightly before 13:41 and gradually declined until its cessation 3 h later. Most of the pumiceous pyroclastic flow deposits were emplaced after the end of the fallout activity at ~16:30 but before the summit caldera collapse at approximately 19:11. Only a small volume of pumiceous flow deposits accumulated after the final caldera collapse. In contrast to the previous reconstruction of Holasek et al. (1996), which interpreted the progressive lowering of the column, documented by satellite data, as due to a decreasing mass eruption rate, we suggest that a progressive shift from a plinian column to a large co-ignimbrite column could also account for such a variation.  相似文献   
138.
139.
A reconstruction is made of the relief which is probably developed through peneplanation and a contemporary deep kaolinisation during late Cretaceous time before the laterite formation and the relief at the time of the laterite formation in Eocene in the region of the present Guiana shield and its foreland. A characteristic plain with very shallow valleys and a thick Al-laterite on its surface was formed during Eocene time. The Al-laterite is used as a characteristic and reference horizon for the post Eocene tectonic which is characterized by a main bulge of the Guiana shield in Surinam, a weaker lift in Guyana and a submergence below sea level in the north.  相似文献   
140.
The aim of this work is to quantitatively set up a simple hypothesis for occurrence of earthquakes conditioned by prior events, on the basis of a previously existing model and the use of recent instrumental observations. A simple procedure is presented in order to determine the conditional probability of pairs of events (foreshock-mainshock, mainshock-aftershock) with short time and space separation. The first event of a pair should not be an aftershock, i.e., it must not be related to a stronger previous event. The Italian earthquake catalog of the Istituto Nazionale di Geofisica (ING) (1975–1995, M 3.4), the earthquake catalog of the Japan Meteorological Agency (JMA) (1983–1994, M 3.0) and that of the National Observatory of Athens (NOA) (1982–1994, M 3.8) were analyzed. The number of observed pairs depends on several parameters: the size of the space-time quiescence volume defining nonaftershocks, the inter event time, the minimum magnitude of the two events, and the spatial dimension of the alarm volume after the first event. The Akaike information criterion has been adopted to assess the optimum set of space-time parameters used in the definition of the pairs, assuming that the occurrence rate of subsequent events may be modeled by two Poisson processes with different rates: the higher rate refers to the space-time volume defined by the alarms and the lower one simulates earthquakes that occur in the nonalarm space-time volume. On the basis of the tests carried out on the seismic catalog of Italy, the occurrence rate of M 3.8 earthquakes followed by a M 3.8 mainshock within 10 km and 10 days (validity) is 0.459. We have observed, for all three catalogs, that the occurrence rate density for the second event of a couple (mainshock or aftershock) of magnitude M2 subsequent to a nonaftershock of magnitude M1 in the time range T can be modeled by the following relationship: (T, M2) = 10a + b(M1 - M2) with b varying from 0.74 (Japan) to 1.09 (Greece). The decrease of the occurrence rate in time for a mainshock after a foreshock or for large aftershocks after a mainshock, for all three databases, obeys the Omori's law with p changing from 0.94 (Italy) to 2.0 (Greece).  相似文献   
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