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141.
石汇平 《地下水》2004,26(2):82-84,139
本文通过对黄土地区潜水含水层深井进行现场单井多落程抽水试验和双井抽水试验资料的整理分析,得到黄土潜水含水层深井抽水井流的一般规律,同时对水跃值的变化规律进行分析.  相似文献   
142.
The crenulated geometry of the Southeast Indian ridge within the Australian-Antarctic discordance is formed by numerous spreading ridge segments that are offset, alternately to the north and south, by transform faults. Suggested causes for these offsets, which largely developed since ~ 20 Ma, include asymmetric seafloor spreading, ridge jumps, and propagating rifts that have transferred seafloor from one flank of the spreading ridge to the other. Each of these processes has operated at different times in different locations of the discordance; here we document an instance where a small (~ 20 km), young (< 0.2 Ma), southward ridge jump has contributed to the observed asymmetry. When aeromagnetic anomalies from the Project Investigator-1 survey are superposed on gravity anomalies computed from Geosat GM and ERM data, we find that in segment B4 of the discordance (between 125° and 126° E), the roughly east-west-trending gravity low, correlated with the axial valley, is 20–25 km south of the ridge axis position inferred from the center of magnetic anomaly 1. Elsewhere in the discordance, the inferred locations of the ridge axis from magnetics and gravity are in excellent agreement. Ship track data confirm these observations: portions of Moana Wave track crossing the ridge in B4 show that a topographic valley correlated with the gravity anomaly low lies south of the center of magnetic anomaly 1; while other ship track data that cross the spreading ridge in segments B3 and B5 demonstrate good agreement between the axial valley, the gravity anomaly low, and the central magnetic anomaly. Based on these observations, we speculate that the ridge axis in B4 has recently jumped to the south, from a ridge location closer to the center of the young normally magnetized crust, to that of the gravity anomaly low. The position of the gravity low essentially at the edge of normally magnetized crust requires a very recent (< 0.2 Ma) arrival of the ridge in this new location. Because this ridge jump is so young, it may be a promising location for future detailed studies of the dynamics, kinematics, and thermal effects of ridge jumps.The U.S. Government right to retain a non-exclusive, royalty-free license in and to any copyright is acknowledged.  相似文献   
143.
跳出南海看南海——新特提斯洋闭合与南海的形成演化   总被引:6,自引:5,他引:1  
本文总结了笔者参与基金委重大研究计划"南海深海过程演变"的研究成果。我们发现南海和青藏高原都是新特提斯洋闭合的产物,而非前人所说的南海是由青藏高原碰撞导致的中南半岛逃逸所形成。与青藏高原碰撞隆升机制不同,南海是新特提斯闭合后期弧后拉张的结果。新特提斯洋位于北边的欧亚大陆与南面的非洲、印度和澳大利亚板块之间,呈东宽西窄的喇叭型。在西部,新特提斯洋向北的俯冲可能在侏罗纪就开始了,局部形成了弧后盆。约130Ma前,由于凯尔盖朗等大火成岩省的喷发,新特提斯洋脊也开始向北漂移。由于新特提斯洋东部宽度较大,弧后拉张明显,形成了古南海。新特提斯洋闭合过程中一个重大事件是洋脊俯冲:从菲律宾经福建及两广到青藏高原,均有100Ma左右的埃达克岩产出,是洋脊俯冲的产物。其中,菲律宾、福建、广东埃达克岩形成了斑岩铜金矿床;而在青藏高原,埃达克岩虽有矿化,但没有形成大规模的斑岩铜金矿床。同时期,华南出现了一次短暂的大规模挤压事件,与洋脊俯冲契合。这次挤压事件可能导致了古南海闭合的开始。与此同时,青藏高原冈底斯出现高温岩石——埃达克质紫苏花岗岩;其北面有~110Ma短时间内发生的大规模花岗岩事件。考虑到板块重建的结果,这些埃达克岩和华南短时间挤压事件的时空分布显示新特提斯洋脊在约100~110Ma,近似平行于俯冲带俯冲到了欧亚大陆之下;其前片下沉,扰动软流圈,形成大规模岩浆活动;后片则缓慢后撤,于~80Ma形成了A-型花岗岩。这些A-型花岗岩多属于A2型,受到了还原性板块俯冲的影响而普遍含锡,形成了全球60%的锡矿。俯冲板片的后撤,导致了拉张,可以合理解释南海北缘的"神狐运动"。随着俯冲板片后撤,俯冲角度加大,形成新的弧后拉张,于~33Ma出现洋壳,形成了南海。青藏高原碰撞引起的物质向东、南、北等各方向逃逸,对东亚大陆的构造格局也产生了重要的影响,但是并非南海拉张的主要控制因素。到~23Ma时,东经九十度海岭的俯冲阻挡了青藏高原下方地幔物质向东南方向逃逸,改变了东亚构造格局。同时,由于该海岭俯冲产生的向北东方向的挤压,造成印支半岛向西南挠曲,导致南海洋脊产生向南的跃迁。  相似文献   
144.
艾比湖流域沙尘气候变化趋势及其突变研究   总被引:25,自引:8,他引:17  
杨青  何清  李红军  雷加强 《中国沙漠》2003,23(5):503-508
通过艾比湖流域5个气象站建站~2001年的观测资料,对艾比湖流域沙尘气候的变化趋势进行了分析。结果表明,气候发生了明显的变化,主要表现在气温升高,降水增多,但分布不均,沙尘暴、扬沙和大风日数稳定减少,但浮尘日数显著上升,风速分布发生了变化,大风日数的迅速减少还引起蒸发能力的减弱。艾比湖干枯的湖底盐漠面积与该流域沙尘总日数之间存在密切关系,艾比湖水域的伸缩而引发的荒漠化环境变化是造成该流域沙尘天气的主要因素。对艾比湖流域沙尘气候的突变检验结果表明,大风、沙尘暴、扬沙日数的减少和浮尘日数的上升是一种突变现象,这种突变与整个西北气候的变化和艾比湖流域沙漠化条件的变化存在一定的关系。  相似文献   
145.
近50年我国江淮流域气候变化   总被引:20,自引:0,他引:20  
为了详实地了解江淮流域的气候变化和进一步做好短期气候预测,利用近50a气温和降水资料,从平均值和变率两方面研究了我国江淮流域的气候变化.结果表明:(1) 近50a来江淮流域气候变化的主要特征是气候变暖,与全国变暖的趋势一致;降水呈不显著的增长趋势.温度和降水由低基本态向高基本态过渡,目前均处于高气候基本态下;(2) 无论是温度还是降水,其变率随时间而变,目前均处于高气候变率时段,要注意高基本态和高变率结合易导致的高温、洪涝等极端气候事件;(3) 温度在1986年前后发生了一次突变,降水在1968年前后发生了一次突变.无论是温度还是降水,突变后均比突变前有所增加.根据突变分析可将江淮流域近50a气候变化过程划分为相对冷干阶段(20世纪50~60年代)-相对冷湿阶段(70~80年代)-相对暖湿阶段(90年代至今).  相似文献   
146.
An analysis has been conducted of the multi-hierarchical structure and jump of temperature variation for the globe, China and Yunnan Province over the past 100 years using an auto-adaptive, multi-resolution data filter set up in You, Lin and Deng (1997). The result is shown below in three aspects. (11 The variation of global temperature in this period is marked by warming on a large scale and can be divided into three stages of being cold (prior to 1919), warm (between 1920 and 1978) and warmer (since 1979). Well-defined jumps are with the variation in correspondence with the hierarchical evolution on such scale, occurring in 1920 and 1979 when there is the most substantial jump towards warming. For the evolution on smaller scales, however, the variation has shown more of alternations of cold and warm temperatures. The preceding hierarchical structure and warming jump are added with new ones. (2) The trend in which temperature varies is much the same for China and the Yunnan Province, but it is not consistent with that globally, the largest difference being that a weak period of cold temperature in 1955-1978 across the globe was suspended in 1979 when it jumped to a significant warming,while a period of very cold temperature in 1955-1986 in China and Yunnan was not followed by warming in similar extent until 1987. (3) Though there are consistent hierarchical structure and jumping features throughout the year in Yunnan, significant changes with season are also present and the most striking difference is that temperature tends to vary consistently with China in winter and spring but with the globe in summer and fall.  相似文献   
147.
煤体性质对煤吸附容量的控制作用探讨   总被引:6,自引:2,他引:4  
煤体性质是影响煤吸附容量的重要因素之一。通过对中国华北和西北两个重要煤层气富集区煤的煤岩学、煤化学和等温吸附实验分析,从煤级、显微组分、煤体变形三个方面对煤的吸附容量及其控制因素进行了, 分析探讨。结果表明,水分平衡条件下煤的吸附容量与煤阶的关系为倒U字型,吸附容量随煤阶的变化为跃变式, 基本与四次煤化作用跃变阶段相对应,主要受控于煤化作用过程中煤的亲甲烷能力和孔隙度的变化;煤体中惰质组含量较高时,其对煤体的吸附容量的影响较为明显,主要与惰质组中丝质体的高吸附能力有关;在构造应力作用下,煤体表面物化发生的变化使构造煤吸附容量比同一矿区同一煤层原生结构煤高。  相似文献   
148.
When nonwetting fluid displaces wetting fluid in a porous rock many rapid pore-scale displacement events occur. These events are often referred to as Haines jumps and any drainage process in porous media is an ensemble of such events. However, the relevance of Haines jumps for larger scale models is often questioned. A common counter argument is that the high fluid velocities caused by a Haines jump would average-out when a bulk representative volume is considered. In this work, we examine this counter argument in detail and investigate the transient dynamics that occur during a Haines jump. In order to obtain fluid–fluid displacement data in a porous geometry, we use a micromodel system equipped with a high speed camera and couple the results to a pore-scale modeling tool called the Direct HydroDynamic (DHD) simulator. We measure the duration of a Haines jump and the distance over which fluid velocities are influenced because this sets characteristic time and length scales for fluid–fluid displacement. The simulation results are validated against experimental data and then used to explore the influence of interfacial tension and nonwetting phase viscosity on the speed of a Haines jump. We find that the speed decreases with increasing nonwetting phase viscosity or decreasing interfacial tension; however, for the same capillary number the reduction in speed can differ by an order of magnitude or more depending on whether viscosity is increased or interfacial tension is reduced. Therefore, the results suggest that capillary number alone cannot explain pore-scale displacement. One reason for this is that the interfacial and viscous forces associated with fluid–fluid displacement act over different length scales, which are not accounted for in the pore-scale definition of capillary number. We also find by analyzing different pore morphologies that the characteristic time scale of a Haines jump is dependent on the spatial configuration of fluid prior to an event. Simulation results are then used to measure the velocity field surrounding a Haines jump and thus, measure the zone of influence, which extends over a distance greater than a single pore. Overall, we find that the time and length scales of a Haines jump are inversely proportional, which is important to consider when calculating the spatial and temporal averages of pore-scale parameters during fluid–fluid displacement.  相似文献   
149.
对比分析了CSRS-PPP、APPS、GAPS、magicGNSS 4款在线PPP服务系统对钟跳数据的处理能力。结果表明,CSRS-PPP的稳健性最好,能够有效处理三类ms级钟跳的数据;APPS能够有效解决第一类ms级钟跳对定位的不利影响,但其对第二类ms级钟跳缺乏必要的控制;GAPS则完全没有顾及钟跳的影响,当发生第一、二类钟跳时,定位结果反复重新初始化,严重影响了PPP的定位精度;magicGNSS的稳健性最差,即便是对于许多不存在钟跳的数据,其定位结果也相对较差,甚至经常出现解算失败的现象。此外,还对计划升级为在线PPP服务系统的TriP 3.0的钟跳处理能力进行了简要分析,结果表明,该软件能够有效处理各类钟跳数据,定位精度较高。  相似文献   
150.
1980年和1981年夏季及其前期冬春季太平洋和印度洋海温均未出现显著异常。然而,这两年东亚夏季风环流的季节内变化却呈现显著异常,且截然不同,具体表征为:1980年西太平洋副热带高压(副高)第一次北跳异常偏早,第二次北跳异常偏晚,而1981年则相反,第一次北跳接近气候态,第二次北跳却异常偏早。就副高两次北跳过程而言,其直接原因也有显著差异:1980年副高两次北跳主要受热带西太平洋对流增强的影响,而1981年两次北跳则是由于热带西太平洋对流增强后所激发的极向传播的Rossby波列与中高纬度东传的Rossby波的锁相作用造成的。与北跳过程相比,副高北跳前后环流稳定维持的时间长短显得更为重要。研究表明,1980年夏季副高异常程度之所以堪比1983年和1998年强El Ni?o衰减年,主要是由于不同阶段南半球环流和北半球中高纬度环流的相互配合与接力,其中,6月和8月副高异常偏强对夏季平均副高异常偏强起到主要贡献,但二者的影响因子不同:6月主要受马斯克林高压(马高)偏强的影响,而8月则与澳大利亚高压(澳高)异常偏强有关。此外,7月和8月副高异常偏南是因为鄂霍茨克海阻塞高压长期维持。与1980年相比,1981年夏季马高和澳高均异常偏弱,因而南半球环流对副高异常的影响有限。北半球中高纬度环流的季节内变化对该年夏季副高的快速北进和南退起主导作用,特别是8月中高纬度盛行强烈的经向环流,使得副高异常偏东偏弱,从而导致夏季平均副高异常偏东偏弱。本文的个例分析表明,在无显著海温异常强迫的年份需要特别关注南半球环流和北半球中高纬度环流对副高及与之相关的东亚夏季风环流的季节内演变的影响,但是这些环流因子持续性较差,难以用于跨季度预测。  相似文献   
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