Structure Refinement of Cs-rich Na-Li Beryl and Analysis of Its Typomorphic Characteristics of Configurations

1 Introduction Natural beryl is an accessory mineral mainly in pegmatite, partly in some highly diffractionated granite or metamorphic rocks, with the crystal shapes beingprismatic, or occasionally tabular. For tabular beryl found in pegmatite it is believed that the tabular configuration is connected with alkali metals (Bieus, 1960; Wang et al., 1981) and geneses of the tabular configuration have been reported before. In recent years, tabular beryl has been found in the Xuebaoding W-Sn-Be d…     

Provenance of Precambrian Fe- and Al-rich Metapelites in the Yenisey Ridge and Kuznetsk Alatau, Siberia： Geochemical Signatures

Major, trace and rare earth element contents of Fe- and Al-rich metapelites from the Korda （Yenisey Ridge） and Amar （Kuznetsk Alatau） formations were determined to examine the nature, origin and evolution of their protoliths. Results indicate that these rocks are the redeposited and metamorphosed products of Precambrian kaolinitic weathering crusts, while the geochemical distinctions between the studied metapelites are determined by different weathering conditions in the source area and tectonic settings. The protolith of the Korda Formation metapelites was produced by erosion products of the post-Archean granitoid rocks, which accumulated under humid climate conditions in shallow-water basins along the continental margin. The geochemical characteristics of the deeper primary deposits of the Amar Formation suggest that volcanogenic material of mafic composition derived from an island-arc environment had a major role in supplying the erosion zone. These results agree with lithofacies data and with the geodynamic reconstruction of the evolution of the Yenisey Ridge and Kuznetsk Alatau during the Mesoproterozoic and Neoproterozoic, respectively. It was shown that REEs had limited mobility during contact metamorphism. The coherent mobility of REEs during collisional metamorphism may be attributed both to mineral reactions responsible for modal changes and to local chemical heterogeneity inherited from the initial protolith.     

基于SEED波形文件的运行率统计

介绍了基于SEED波形文件运行率计算的技术和实现方法,介绍了SEED文件中标识时间的特殊掩码、时间片的具体格式和程序的实现,并给出了与其相关的部分源代码.     

分层强夯联合电渗法处理疏浚淤泥宏细观试验研究

为提高强夯联合电渗法处理疏浚淤泥的效果,提出了分层强夯联合电渗法处理疏浚淤泥的方法。设计了4组室内模型试验,分别采用纯电渗、分1层、2层及3层强夯联合电渗法对疏浚淤泥进行处理,研究分层强夯联合电渗法的处理效果,并通过扫描电镜分析了试验后阴极附近土体的孔隙特征。结果表明：分层强夯联合电渗法加固效果优于纯电渗法,且分层数越多、促进效果越好;分3层强夯的排水量达到6.35 kg、电流强度的衰减得到了较好的抑制效果;分3层强夯比纯电渗法的排水量增加了37.15%,十字板剪切强度增加了41.42%;电镜扫描结果显示,分3层强夯时阴极附近的土体裂缝明显减少,均一化程度最高。     

2014年夏季长江流域持续性低温的大尺度环流异常

采用中国地面站气温逐日观测资料、NOAA全球逐日海表温度资料,及NCEP/NCAR的全球日均再分析资料,研究了2014年持续性低温的三维结构及大尺度环流异常。结果表明,2014年的低温异常,除了在陆地上区域性地出现在长江流域,还以大尺度带状的形式、从陆地延伸到海洋上。这种带状异常不只出现在近地面,在大气各层（925～500 hPa）都能看到。分析指出,大气中的这个低温带主要由高纬大气环流异常造成。在位势高度场上,最重要的异常出现在高纬60°N,有呈带状的位势高度正距平,它引导（距平意义上的）偏北气流从正北和东北偏东方向侵入,在其南侧形成一带状的偏低温区。大气各层均呈现出这种在高纬有位势高度正距平、相应地在稍南的低纬（40°N）有位势高度负距平、两者之间为低温区的分布特征。从低层往上,这种配置型式整体表现出由南往北的倾斜,其垂直剖面表现为距平意义上的、大尺度、类似于锋面的倾斜结构。文中用简单的概念模型对此进行理解,认为这种结构是由大气动力异常和热力异常相互影响、共同作用而形成的。     

金沙江白鹤滩水电站坝址区断层变形特点及成因分析

拟建中的白鹤滩水电站坝基将建在二叠系峨眉山组玄武岩层之上.坝址区发育有位移量较小的NW300°、NW320°、NE40°和近SN向4组断层,其中NW300°断层最为发育.在野外详细调查的基础上,室内的显微构造研究和电子自旋共振(简称ESR)测年结果表明,坝址区内的断层是在燕山期晚期近东西向挤压应力场作用下形成,后期又受到了近南北向挤压应力场的改造.断层破碎带以发育典型碎裂-角砾岩等浅层脆性构造岩为特点,近期活动不明显.     

天津静海-津南剖面地壳上地幔电性结构特征

在天津市区南部的静海-津南一线布置了32个大地电磁测深点,剖面方位角92°,对采集的资料采用远参考与Robust技术进行了处理和解释.对该区的构造维数及构造方向做了分析,揭示了该剖面地壳上地幔电性结构特征,并进行了划分.成果显示:中下地壳存在双层低阻构造层,上地幔表现为中、高阻互层.在断裂带附近受构造活动影响,低阻高导构造层会发生上下错断与缺失.沧东、白塘口、天津断裂均是多组断层构成的断裂带,控制了双窑凸起、白塘口凹陷、板桥凹陷及静海斜坡带次级构造单元.     

隔震建筑结构的强震观测与初步分析

福建省防灾减灾隔震大楼自2005年8月架设强震观测结构台阵以来,已多次记录到大楼地震动力反应,这些宝贵的结构反应资料对于评价隔震效果、分析结构反应特性具有十分重要的价值。本文从中选取了震级在3.7~7.6、震中距在189~3 595km的24次地震的台阵资料,对大楼的振动特性和隔震效果进行了初步分析,得到的结论是:(1)大楼场地土层的特征周期在0.63~0.68 s;(2)中心大楼在小地震作用下表现的振动卓越频率分别为4.7Hz(垂直向)、1.31Hz(南北向)、1.40Hz(东西向),大楼水平向第一阶振型的频率分别为1.41Hz(南北向)、1.59Hz(东西向),即自振周期为0.70 s(南北向)、0.63 s(东西向);(3)大楼在小地震时隔震效果不明显,其南北向隔震效果比东西向好;随着地下室记录峰值的增大,顶层放大倍数有所降低,大楼卓越频率也有所降低;(4)初步分析表明大楼在小震时仍有扭转效应,其扭转周期为0.5 s,有待进一步分析。     

Loss of energy dissipation capacity from the deadzone in linear and nonlinear viscous damping devices

In a viscous damping device under cyclic loading, after the piston reaches a peak stroke, the reserve movement that follows may sometimes experience a short period of delayed or significantly reduced device force output. A similar delay or reduced device force output may also occur at the damper’s initial stroke as it moves away from its neutral position. This phenomenon is referred to as the effect of “deadzone”. The deadzone can cause a loss of energy dissipation capacity and less efficient vibration control. It is prominent in small amplitude vibrations. Although there are many potential causes of deadzone such as environmental factors, construction, material aging, and manufacture quality, in this paper, its general effect in linear and nonlinear viscous damping devices is analyzed. Based on classical dynamics and damping theory, a simple model is developed to capture the effect of deadzone in terms of the loss of energy dissipation capacity. The model provides several methods to estimate the loss of energy dissipation within the deadzone in linear and sublinear viscous fluid dampers. An empirical equation of loss of energy dissipation capacity versus deadzone size is formulated, and the equivalent reduction of effective damping in SDOF systems has been obtained. A laboratory experimental evaluation is carried out to verify the effect of deadzone and its numerical approximation. Based on the analysis, a modification is suggested to the corresponding formulas in FEMA 356 for calculation of equivalent damping if a deadzone is to be considered.     

Joint probability density function of the stochastic responses of nonlinear structures

The joint probability density fimction （PDF） of different structural responses is a very important topic in the stochastic response analysis of nonlinear structures. In this paper, the probability density evolution method, which is successfully developed to capture the instantaneous PDF of an arbitrary single response of interest, is extended to evaluate the joint PDF of any two responses. A two-dimensional partial differential equation in terms of the joint PDF is established. The strategy of selecting representative points via the number theoretical method and sieved by a hyper-ellipsoid is outlined. A two-dimensional difference scheme is developed. The free vibration of an SDOF system is examined to verify the proposed method, and a flame structure exhibiting hysteresis subjected to stochastic ground motion is investigated. It is pointed out that the correlation of different responses results from the fact that randomness of different responses comes from the same set of basic random parameters involved. In other words, the essence of the probabilistic correlation is a physical correlation.