凌汛期槽蓄水增量过程模拟

为研究凌汛期槽蓄水增量来源,在分析实测冰情资料基础上,把槽蓄水增量分为水位壅高主河道蓄水量增大、主河道内河水转化为固体冰盖和上滩水形成冰盖及在冰下聚集等3部分,建立河冰动力学模型,模拟河冰生消及槽蓄水增量过程,利用2008/2009年度三湖河口—头道拐河段实测冰情资料对模型进行了验证,表明滩地冰盖及冰盖下滞洪是内蒙古河段槽蓄水增量的主要来源,占最大槽蓄水增量的63.44%,主河道水位壅高引起的槽蓄水增量占26.56%,主槽冰盖蓄水占10.0%。     

阿尔金南缘地质填图新进展及对找矿的启示——据甘肃1:5万莫坝尔等六幅区调

通过开展甘肃1∶5万莫坝尔等六幅区域地质调查工作,系统查明了区域地层、岩石、构造等地质特征和成矿地质条件,建立了区内地层格架和岩浆岩演化序列,查明了测区基本构造格架,并总结了本区的构造演化历史;新发现余石山大型铌钽稀有金属等矿床和矿(化)点24处,在此基础上在测区划分出找矿前景较好的4个成矿远景区,为后续找矿工作提供了基础地质资料。     

深度学习方法在北极海冰预报中的应用

在全球气候变暖背景下,北极海冰呈现出逐年消融的趋势.海冰的消融给北极的开发利用带来了重要机遇,例如北极航道通航潜力的显现.但北极航道开通还面临着诸多困难,尤其是海冰变化机理的复杂性和海冰预报的不确定性以及由此带来的航行安全风险.近年来,深度学习因其强大的非线性拟合能力,逐渐在海冰预报领域中崭露头角.本文对近年来深度学习...     

白令海盆17ka以来的古海洋与古气候记录

通过白令海盆08BR02钻孔(57°0.06'N,174°29.97'E,水深3 805 m)的AMS14C测年数据、颜色反射率b*与NGRIP(North Greenland Ice Core Project)氧同位素曲线及白令海4个钻孔颜色反射率b*记录作对比,建立该孔的地层年代框架,顶、底部沉积物年龄分别为4.2 ka和17.0 ka。该孔自17 ka以来,IRD(ice-rafted detritus:冰筏碎屑)、粒度的砂组分以及敏感组分中的33—63μm组分百分含量在全球性冷事件H1(Heinrich event 1)、B/A(Blling/Allerd)中期和YD(Younger Dryas)期间明显增加。IRD和有孔虫丰度在H1、B/A和YD期间同步增加,可能反映海冰融化为表层水提供营养物质,促使表层钙质生产力勃发并将有机质进一步输送至海底,为底栖生物提供营养物质。     

南极冰盖地形数据库BEDMAP 2述评

南极冰盖物质收支与不稳定性对全球气候变化和海平面升高有着重要影响,而冰盖厚度和冰下地形则是研究南极冰盖的物质平衡、动力及不稳定性极为重要的参数。自20世纪50年代以来,国际上针对南极冰盖开展了大量的冰雷达以及重、磁测量,这些测量结果被汇集并形成冰厚和冰下地形数据库,进而服务于冰盖模式和地球系统研究,最新推出的成果便是BEDMAP 2(Bedrock Mapping Project 2)。首先介绍了BEDMAP 2的数据来源、结构以及数据处理,并讨论了数据的质量评价,然后分析了BEDMAP 2中展示的整个南极冰盖与冰下地形及其特点。最后,对于BEDMAP 2对中国在南极冰盖考察和研究方面的作用进行了一些讨论与展望。     

夏季南大洋南极大磷虾种群分布、结构及生长研究

利用2007/2008年和2008/2009年南极夏季高速采集器和IKMT网走航采样样品,结合同步环境调查资料,研究了南极大磷虾(Euphausia superba)的水平分布、生长状况及种群结构。结果表明,南极大磷虾在威德尔海域丰度高于普里兹湾海域,两个海域的磷虾丰度都低于历史同期。从两个年度南极考察的整个调查海区来看,南极大磷虾处于正常生长状态,但也存在个别生长状况较差站位,推测与海冰回退时间较晚或叶绿素浓度较低有关。利用高速采集器采集的大磷虾样品,在海冰边缘区域站位,未成体磷虾占有很大比例;而在海冰已经消退较长时间的海域,成体磷虾占比例较大,这反映了大磷虾未成体与成体不同的分布特征。南极大磷虾在不同海域种群结构存在一定的差异,对种群补充产生一定的影响。     

Advances in thermokarst lake research in permafrost regions

A thermokarst lake is defined as a lake occupying a closed depression formed by ground settlement following thawing of ice-rich permafrost or the melting of massive ice. As it is the most visible morphologic landscape developed during the process of permafrost degradation, we reviewed recent literature on thermokarst studies, and summarized the main study topics as： development and temporal evolution, carbon release, and ecological and engineering influence of thermokarst lakes. The climate warming, forest fires, surface water pooling, geotectonic fault and anthropogenic activity are the main influencing factors that cause an increase of ground temperatures and melting of ice-rich permafrost, resulting in thermokarst lake formation. Normally a thermokarst lake develops in 3–5 stages from initiation to permafrost recovery. Geo-rectified aerial photographs and remote sensing images show that thermokarst lakes have been mainly experiencing the process of shrinkage or disappearance in most regions of the Arctic, while both lake numbers and areas on the Qinghai-Tibet Plateau have increased. Field studies and modeling indicates that carbon release from thermokarst lakes can feedback significantly to global warming, thus enhancing our understanding of the influences of thermokarst lakes on the ecological environment, and on regional groundwater through drainage. Based on field monitoring and numerical simulations, infrastructure stability can be affected by thermal erosion of nearby thermokarst lakes. This review was undertaken to enhance our understanding of thermokarst lakes, and providing references for future comprehensive studies on thermokarst lakes.     

Changes to the Canadian Arctic Archipelago Sea Ice and Freshwater Fluxes in the Twenty-First Century under the Intergovernmental Panel on Climate Change A1B Climate Scenario

A coupled ocean and sea-ice pan-Arctic model forced by the Intergovernmental Panel on Climate Change A1B climate scenario is used to study the evolution of ice and ocean surface conditions within the Canadian Arctic Archipelago (CAA) during the twenty-first century. A summer ice-free CAA is likely by the end of our simulation. Sea ice undergoes significant changes from the mid-2020s to the mid-2060s in both concentration and thickness. The simulation shows a shrinking of 65% and a thinning of 75% in summer over the 40 years, resulting in a partially open Northwest Passage by the 2050s. However, ice in central Parry Channel might increase due to a decrease in export from April to June, linked to a reduced cross-channel sea surface height (SSH) gradient, before melting thermodynamically. On a larger scale, the central CAA throughflow will experience a significant decrease in both volume and freshwater transport after 2020, which is related to the change in the SSH difference between the two ends of Parry Channel, particularly the lifting of SSH in Baffin Bay. With a lower albedo, a warmer ocean is simulated, particularly in summer. The sea surface salinity within the CAA demonstrates a strong decadal oscillation without a clear trend over the entire simulation. A north–south pattern, separated by Parry Channel, is also found in the changes of ocean temperature and salinity fields due to different ice conditions.     

基于水下光纤应变监测的导管架结构总冰力测量方法

基于测量结构水下光纤应变获取冰力的方法首次应用于渤海JZ20-2NW加锥导管架平台,该方法方便进行零点标定,可获取结构总冰力的绝对信息(包括均值和波动值)。首先介绍了JZ20-2NW平台的现场监测系统,主要包括结构水下应变响应记录冰力信息,甲板上部视频记录同步冰情(冰厚、冰速和来冰方向)信息和拾振器记录结构冰振响应;重点分析了由测点应变向结构总冰力的转化方法,并对总冰力进行了初步分析。将无量纲化实测冰力与5种典型冰力计算模型进行了比较,分析结果表明,锥体宽度与海冰厚度比值(简称"宽厚比")对冰力大小及变化起决定作用。     

Modelling argon dynamics in first-year sea ice

Focusing on physical processes, we aim at constraining the dynamics of argon (Ar), a biogeochemically inert gas, within first year sea ice, using observation data and a one-dimensional halo-thermodynamic sea ice model, including parameterization of gas physics. The incorporation and transport of dissolved Ar within sea ice and its rejection via gas-enriched brine drainage to the ocean, are modeled following fluid transport equations through sea ice. Gas bubbles nucleate within sea ice when Ar is above saturation and when the total partial pressure of all three major atmospheric gases (N₂, O₂ and Ar) is above the brine hydrostatic pressure. The uplift of gas bubbles due to buoyancy is allowed when the brine network is connected with a brine volume above a given threshold. Ice-atmosphere Ar fluxes are formulated as a diffusive process proportional to the differential partial pressure of Ar between brine inclusions and the atmosphere. Two simulations corresponding to two case studies that took place at Point Barrow (Alaska, 2009) and during an ice-tank experiment (INTERICE IV, Hamburg, Germany, 2009) are presented. Basal entrapment and vertical transport due to brine motion enable a qualitatively sound representation of the vertical profile of the total Ar (i.e. the Ar dissolved in brine inclusions and contained in gas bubbles; TAr). Sensitivity analyses suggest that gas bubble nucleation and rise are of most importance to describe gas dynamics within sea ice. Ice-atmosphere Ar fluxes and the associated parameters do not drastically change the simulated TAr. Ar dynamics are dominated by uptake, transport by brine dynamics and bubble nucleation in winter and early spring; and by an intense and rapid release of gas bubbles to the atmosphere in spring. Important physical processes driving gas dynamics in sea ice are identified, pointing to the need for further field and experimental studies.