Summer fast ice evolution off Zhongshan Station,Antarctica

Based on the field data acquired in the program of fast ice observation off Zhongshan Station, Prydz Bay, East Antarctica during the austral summer 2005/ 2006, physical properties evolution of fast ice during the ice ablation season is analyzed in detail. Results show that the annual maximum ice thickness in 2005 occurred in later November, and then ice started to reek, and the ablation duration was 62 days; sea water under the ice became warmer synchronously; corresponding to the warming sea ice temperature, a ＂relative cold mid-layer＂ appeared in sea ice; the fast ice marginal line recoiled back to the shore observably, and the recoil distance was 20.9 km from 18 December 2005 through 14 January 2006. In addition, based on the data of sea ice thickness survey along the investigation course of MV Xuelong on December 18 of 2005, the ice thickness distribution paten in the marginal ice zone have been described ： sea ice thickness increased, but the diversity of floe ice thick-ness decreased from open water to fast ice zone distinctly.     

Crystals and fabrics analysis of an Arctic thermal growth multi-year ice sample

One of sea ice core samples was taken from Arctic by the First Chinese National Arctic Research Expedition Team in 1999. 20 vertical and 2 horizontal ice sections were cut out of the ice core sample 2.22 m in length, which covered the ice sheet from surface to bottom except losses for during sampling and section cutting. From the observation and analysis of the fabrics and crystals along the depth of the ice core sample, followings were found. Whole ice sheet consists of columnar, refrozen clastic pieces, granular, columnar, refrozen clastic pieces, granular, columnar and refrozen clastic pieces. This indicates that the ice core sample was 3-year old, and the ice sheet surface thawed and the melt water flowed into ice sheet during summer. Hence, the annual energy balance in Arctic can be determined by the ice sheet surface thawing in summer, and bottom growth in winter. The thickness of the ice sheet is kept constantly at a certain position based on the corresponding climate and ocean conditions; A new     

西藏冈底斯南缘汤白矿区早侏罗世含矿斑岩锆石U-Pb定年及其地质意义

汤白矿区位于西藏冈底斯斑岩铜矿带西段南缘,南侧紧邻日喀则弧前盆地。矿区由地表探矿工程控制3条赋存于早侏罗世角闪石英闪长斑岩中的主矿体(1号、2号和3号),在野外地质调查的基础上,对角闪石英闪长斑岩进行LA-ICP-MS锆石U-Pb定年和岩石地球化学测试。研究结果表明:(1)含矿斑岩的成岩年龄为183.3±1.2Ma,形成于早侏罗世;(2)含矿斑岩地球化学特征与大洋岛弧背景下的安山质岩石的地球化学性质一致,表明汤白矿区含矿斑岩形成于大洋岛弧环境;(3)西藏冈底斯斑岩铜矿带具有寻找俯冲期斑岩型矿床的巨大潜力,今后应加强该带俯冲期斑岩型矿床的勘查评价工作,特别是早—中侏罗世斑岩的成矿潜力评价。     

细粒酒精模型冰的弯曲强度试验研究

基于不同制冰条件和工的细粒酒精模型冰层原位悬臂弯曲强度试验,给出细料酒精模型冰弯曲强度;分析了考虑和不考虑不浮力效应对弯曲强度的差异;利用向睡向下弯曲强度结果给出该模型冰各向同性的证据;得到该冰弯曲强度与其密度、冰内未冻液含量和制冷过程可控制因子的关系,并作为定量控制模型冰质量的基础。     

西安地热井施工技术和成井工艺

西安地热田自开发十多年来,先后有十多个单位施工成井近百口。尽管设备钻具各不相同。施工、成井工艺亦有较大差别,但笔者认为以石油成套钻井设备和石家庄煤机厂的TSJ－2000钻机成套设备施工的热井较具优势。l地层条件西安地热田位于西安凹陷区内。西安凹陷是汾谓盆地三大凹陷之一,面积约2700km‘。基底为震旦亚界片岩及燕山期花岗岩。盖层最厚达70corn,自下而上发育有下第三系红河组、白鹿原组、甘河组、上第三系冷水沟组、寇家村组、兰田。渡河组、张家坡组、第四系三门组、秦川群。应当说明的是：不同构造单元,地层的发育情况差异…     

浮冰界面融化速率参数化方案的实验室研究

融冰季节时天然浮冰表面、底面和侧向融化共存,三者融化速率是底面大于侧向,侧向大于表面。而且浮冰尺寸越小,侧向速率占比越高。为了解决将小尺度浮冰块尺度指标计入融化参数化方案,在低温环境实验室无辐射、无流速、控制气温和水温条件下对天然海冰和人工冻结淡水冰的圆盘试样,开展了不同初始水温和不同初始直径的圆盘试样融化过程实验,获得了圆盘试样直径、厚度和质量融化过程。依据这些实验数据,构建试样直径厚度比这一新指标,通过物理分析和数学统计手段,建立了海冰和淡水冰试样表面、底面融化速率同温度梯度,侧向融化速率和温差以及直径厚度比的关系式。这些关系式能够应用于天然直径100 m范围内浮冰的融化参数化方案,期望能解决北冰洋海冰和入海口近岸淡水冰夏季融化季节能量和质量平衡数值模拟的需求。     

海鞘中的抗肿瘤生物活性物质

综述了海鞘中发现的数十种抗肿瘤活性物质,包括其活性、来源等,对其中重要者,如Ecteinascidians 743和Psedodistomins D-F等活性物质抗肿瘤的作用机理作了较详细的介绍,并概述了国内该领域的研究状况。     

水库地震监测与预测技术研究项目实施情况

介绍了"水库地震监测与预测技术研究"项目在广东河源新丰江水库库区详细的实施情况,包括观测场址的勘选、台基测试、台站建设、仪器安装、数据处理等工作,总结了项目成功实施的经验。     

定点冰厚观测新技术研究

冰厚是冰科学和冰工程研究中最关键的物理指标之一,为满足定点冰厚观测不同需要,发展了3种定点冰厚观测新技术。结合它们的测量原理及其现场或实验室的应用结果,论述了它们的适用性和各自的优点。基于磁致伸缩原理的冰厚测量仪现场测量精度达±2mm,解决了制约海冰热力学模式向精细发展的"瓶颈"问题;电阻式冰厚测量仪比利用温度廓线推求冰厚的技术更加可靠,且具有自动测量冰川表面物质平衡,进行河道、湖泊以及水库冰厚观测时同时监测其冰下水位的潜力;热电阻丝冰厚测量装置制作简单廉价、使用方便、数据可靠,在中国北方小型水文站广泛推广是适合的。     

西藏冈底斯成矿带南缘新特提斯洋俯冲期成矿作用: 来自雄村矿集区Ⅰ号矿体的Re-Os同位素年龄证据

雄村矿集区是近年来西藏冈底斯成矿带内发现的一处超大型铜金矿集区, 该矿集区位于冈底斯造山带中段南缘, 其南侧紧邻日喀则弧前盆地.最新的勘探资料表明, 雄村矿集区由Ⅰ、Ⅱ、Ⅲ号斑岩型铜金矿体组成.本文以雄村Ⅰ号矿体为研究对象, 获得Ⅰ号矿体中4件辉钼矿样品的Re-Os模式年龄范围非常一致, 其变化范围为160.1±2.3~163.4±2.3 Ma, 等时线年龄为161±11 Ma(MSWD=4.2), 误差较大, 而平均模式年龄161.5±2.7 Ma(MSWD=2.0), 误差较小.因此, 雄村Ⅰ号矿体的形成时代为160.1±2.3~163.4±2.3 Ma, 最有可能的形成年龄应为161.5±2.7 Ma, 该年龄代表了雄村Ⅰ号矿体的成矿年龄, 这与前人获得的含矿斑岩(含眼球状石英斑晶的角闪石英闪长玢岩)的锆石U-Pb年龄(164.3±1.9 Ma)基本吻合, 表明矿床形成于中侏罗世.同时, 雄村Ⅰ号矿体的含矿斑岩体和赋矿火山岩具有与岛弧火成岩类似的地球化学特征, 如相对富集LREE、LILE, 亏损HREE、HFS, 缺少或微弱负Eu异常.综合来看, 雄村Ⅰ号矿体形成于新特提斯洋俯冲期(>65 Ma), 产出的构造背景为新特提斯洋向北俯冲形成的岛弧环境, 属岛弧型斑岩铜金矿床.