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基于Landsat-8 OLI影像的天山南伊内里切克冰川2016年冰川表面运动状态提取与分析 总被引：1，自引：1，他引：0
利用Landsat-8 OLI传感器获取的2016年3-9月覆盖天山西段托木尔峰-汗腾格里地区的3期光学遥感影像数据,基于频谱归一化互相关算法提取并分析了该地区南伊内里切克冰川在最近一年消融期内不同时段的表面运动速度分布及其时空变化特征。研究结果表明：2016年消融期内靠近该冰川上游区域可观测到约为55 cm·d-1最大运动速度;由于受到冰川下游物质补给量减弱、表碛物增多等因素影响造成冰川末端区域运动速度最小,整个消融期内冰川主体运动速度基本介于20~50 cm·d-1之间,其平均运动速度约为35 cm·d-1。而且,可观测到位于冰川上游区域在2016年3月9日至9月17日时段内,冰川运动速度呈递增趋势,相反位于冰川下游区域冰川运动速度呈现减弱趋势。另外,与早期研究对比可知,该冰川运动速度有所减缓且冰川末端明显处于退缩状态。 相似文献
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合成孔径雷达(synthetic aperture radar, SAR)具有其全天候、全天时、穿云透雾的工作能力, 广泛应用于山地冰川动态监测中. 利用2006年6-9月三期ALOS/PALSAR雷达影像, 采用偏移量跟踪技术, 提取了喜马拉雅山珠穆朗玛峰(珠峰)区域的冰川运动速度, 分析了区域内冰川运动速度空间差异及其影响因素. 结果表明: 研究区31条山谷冰川平均运动速度为9.3 cm·d-1, 总体上以珠峰-洛子峰南北向山脊线为界限, 东侧和东南侧冰川日均运动速度(11.1 cm·d-1)普遍高于北部和西北部冰川日均运动速度(5.4 cm·d-1). 冰川消融区非表碛区冰川平均运动速度为表碛覆盖区平均运动速度的2.2倍, 冰面湖的发育在一定程度上加剧冰川运动速度波动. 在气候与非气候因子共同作用和相互间的此消彼长中, 研究区65%的冰川的运动速度自中值高度往下显著减小, 16%的冰川自中值高度往下呈显著增大趋势, 19%冰川消融区运动速度无显著变化趋势. 相似文献
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冰川运动速度研究： 方法、 变化、 问题与展望 总被引：3，自引：2，他引：1
冰川运动将积累区获得的物质输送到消融区, 维持着冰川的动态平衡。近年来, 随着气候变化, 全球大部分冰川面临着剧烈的退缩, 而冰川运动变化则较为复杂, 引起了学者们的广泛关注。文章系统总结了近年来冰川运动速度的提取方法、 冰川运动速度时空分布与变化及其影响因素的相关研究进展。另外, 还探讨了目前冰川运动速度研究中存在的问题和未来的发展趋势。结果表明： 基于测杆的方法能够获得精度较高的测量数据, 但存在时间和空间上的局限性; 基于遥感数据自动化提取的方法应用广泛, 但影像之间的配准以及海量数据的计算是当前阶段制约冰川运动速度研究的主要问题; 近年来, 无人机和地基合成孔径雷达的应用为冰川运动速度研究提供了高精度的数据支撑, 但二者在冰川运动研究中的应用还不够广泛。冰川运动速度的分布及其变化在空间上存在明显差异, 冰川厚度的变化可能是全球大部分冰川运动速度变化的主要原因, 但在单个冰川系统上, 冰川运动速度变化较为复杂, 其原因还需要进一步探讨。遥感数据的不断丰富, 云计算平台的使用, 物联网、 无人机和地基合成孔径雷达等技术的不断普及, 以及星、 空、 地协同观测的出现将会极大促进未来冰川运动速度研究的发展。此外, 冰川动力学过程也将备受关注, 成为未来冰川运动研究的热点问题。 相似文献
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SAR偏移量技术和光学偏移量技术是冰川运动监测重要的技术手段,但目前对于融合不同平台的影像进行三维形变的研究较少。文章选取2019年11月至2021年1月西藏聂拉木县希夏邦马峰地区的大型冰川作为研究对象,基于方差分量估计融合该研究区的Sentinel-1与Landsat8两种数据进行冰川的三维位移解算,选取了同一时期的光学影像对偏移量估计结果进行对比分析,同时选取稳定区域进行精度评估,分析该方法在冰川运动监测中的适用性和精确性。结果表明,该冰川在2019年11月至2021年1月,联合解算的东西向最大流速为21 cm/d,南北向最大流速为68 cm/d,垂直向最大流速为17 cm/d。对比单一影像获取的冰川位移结果,多影像联合解算方法,能够弥补SAR数据的失相干和光学数据的低质量像元值的不足,获得更加完整和详细的冰川信息,监测结果精度更高。可为利用不同平台的数据联合监测山地冰川的多维度和高精度变化提供参考和技术支持。 相似文献
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为了保持对祁连山七一冰川运动变化情况观测的连续性,进一步揭示全球气候变暖背景下山岳冰川的运动变化规律,对布设在七一冰川表面的花杆进行了定期观测,获取了2012年7-8月以及2013年8-9月冰川考察期间的最新观测数据（花杆位置、冰川末端边界以及物质平衡等数据资料）,通过对数据进行分析,获得了七一冰川表面的运动状况以及末端进退变化情况. 结果表明：空间分布特征方面,七一冰川在横剖面以及纵剖面的运动保持了一般山岳冰川的运动规律;横剖面上,主流线附近冰川运动速度较两侧运动速度要大;纵剖面上,由冰川末端到零物质平衡线,冰川运动速度逐渐增大;运动方向上,七一冰川运动速度矢量大多沿主流线向下运动,或者稍微偏离主流线一定方向. 在冰川运动速度时间分布特征方面,七一冰川在消融季与非消融季的运动速度差异显著,消融季运动速度要明显大于非消融季运动速度. 最近几十年,七一冰川整体运动速度呈现出了逐年减小的趋势. 在2012年8月至2013年8月期间,冰川末端退缩了大约5～7 m,退缩较为显著. 相似文献
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喀喇昆仑山克勒青河谷近年来发现有跃动冰川 总被引：6，自引：3，他引：3
根据冰川编目、Landsat MSS/TM/ETM 影像和相关的历史考察制图,利用GIS进行了不同时期的冰川分布图的制作,对比分析了不同时期冰川范围.重点监测了喀喇昆仑山北坡克勒青河的5Y654D48、5Y654D97的不同时段内的冰川运动状况.结果发现:5Y654D48冰川和5Y654D97冰川分别在1990-2000年与1977-1990年间运动速度达272 m·a-1,213.1 m·a-1,比其它时段运动速度大7～20倍,具备跃动冰川的运动特征.分析认为,5Y654D48冰川在1990-2000年、5Y654D97在1977-1990年间曾分别发生过冰川跃动. 相似文献
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冰川运动速度对气候变化的响应—以天山乌鲁木齐河源1号冰川为例 总被引：5，自引：1，他引：4
山地冰川对气候变化的响应最为敏感, 在全球变暖的大背景下山地冰川和极地冰盖正在发生显著的变化。冰川运动速度的变化是气候变化的结果之一。乌鲁木齐河源1号冰川是中国西部山地冰川的代表, 本文以1981-2007年27a的运动速度资料与1982年以来的季节运动速度资料为基础, 结合冰川物质平衡、气温、降水等资料分析冰川运动速度对气候变化的响应。研究发现, 27a来1号冰川运动速度下降趋势明显, 冬、夏季节运动速度波动较大, 但夏季运动速度较大。气候变化通过冰川物质平衡的改变作用于冰川运动速度, 物质平衡的持续亏损最终导致了冰川运动速度的持续降低。夏季的高温与降水对冰川运动速度具有加速的作用。 相似文献
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祁连山东段冷龙岭北坡冰川融水是河西走廊重要的水源补给,然而却少有现代冰川运动观测资料. 通过在该区域宁缠河1号和水管河4号冰川布设花杆,观测了冰川表面的运动速度. 结果表明：2010-2012年,面积较大的水管河4号冰川表面年平均运动速度(5.2 m·a-1)要高于面积相对较小的宁缠河1号冰川(2.8 m·a-1). 水管河4号冰川最大运动速度出现在花杆观测区域的最上部(接近物质平衡线),宁缠河1号冰川最大运动速度出现在坡度较大的区域,说明冰川最大运动速度通常出现在平衡线附近,但还要考虑坡度等地形因素的影响. 较之早期的观测资料,水管河4号和其他中国西部地区冰川的运动速度呈现出减缓趋势,可能是物质平衡持续亏损导致冰川厚度变薄的直接结果. 相似文献
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冰川流速是冰川动力状况的重要标志,利用合成孔径雷达技术能快速获得大范围冰川的表面流速.利用日本高级陆地观测卫星(ALOS)相控阵型合成孔径雷达L波段(PALSAR)及欧洲太空局的ENVISAT/ASAR数据的特征匹配方法获得帕米尔高原公格尔山区冰川表面流速,并结合合成孔径雷达干涉相干与不同时期数字高程模型对公格尔山区典型冰川动力进行分析,获得研究区不同时间基线冰川表面相干性、表面流速以及基于不同时相DEM的典型冰川表面高程变化信息.结果表明:30 a来克拉牙依拉克冰川表面高程下降了(15±12.1)m,表碛区域近期运动速度变化不大;其木干冰川平均表面高程几乎无变化,但2007-2011年夏季表面流速明显减缓,靠近末端附近部分区域可能已经演化为非活动区;姜满加尔冰川位于西风带的迎风坡,积累区面积大,冰川流速较快,无表碛覆盖,但表面高程仍下降了(8.8±12.7)m.编号为5Y663D0009的冰川冰舌表碛覆盖区可能已经演化为非活动区,30 a来表面高程下降(8.6±12.0)m.综合分析表明,冰川规模特别是积累区面积的大小及所处位置、地形对冰川演化具有重要影响. 相似文献
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新疆帕米尔跃动冰川遥感监测研究 总被引：11，自引：7，他引：4
2015年5月,新疆克孜勒苏柯尔克孜自治州阿克陶县公格尔九别峰北坡克拉牙依拉克冰川发生跃动,造成草场和部分房屋被冰体淹没,本文针对这一冰川跃动事件的发生过程进行研究.利用2013-2015年间ASTER立体像对数据监测了克拉牙依拉克冰川的冰川表面高程的变化,并利用2015年4月13日至2015年7月11日期间的LandsatOLI数据监测了冰川的表面运动速度变化.监测发现,克拉牙依拉克冰川从2015年4月13号开始活动强烈,表面运动速度呈加快趋势,2015年5月8-15日期间冰川表面运动速度达到最高水平,其最大运动速度在西支中部达到了(20.40±0.42)m·d-1,冰川跃动达到顶峰.冰川跃动"积蓄区"位于西支冰川平衡线以下区域,跃动向下游接收区输送冰体体积约为2.4×108m3,大量冰体堆积在东西支汇合口地段(海拔3100~3500m),造成了该处冰面隆起,其中最大隆起高度为(130.58±0.70)m.本文获得了西支冰川由静止期、跃动状态、恢复到稳定状态期间的冰面高程和表面运动速度变化,为本地区冰川跃动机理的研究奠定了基础. 相似文献
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KNUT STALSBERG EILIV LARSEN DAG OTTESEN HANS PETTER SEJRUP 《Boreas: An International Journal of Quaternary Research》2003,32(1):149-166
Glacial lineations on a bank area and a coastal lowland, both bordering the Norwegian Channel, are studied with regard to morphology and distribution by means of side-scan sonar data, detailed digital maps and fieldwork. Their genesis and age are further elucidated through stratigraphic and sedimentologic information from excavations in one typical coast-parallel drumlin. Four excavated sections revealed four lithologic units: Prodeltaic glaciomarine sand, glaciofluvial gravel, glaciomarine diamicton and deformation till. After Middle Weichselian delta progradation, glaciomarine diamicton was deposited and later subglacially reworked by a northwards flowing glacier. The two upper diamictons form the main volume of the ridge, which is interpreted as a drumlin, and imply a reinterpretation of the Jæren part of the so-called Lista moraine. Preconsolidation of glaciomarine diamicton suggests a maximum ice thickness of 500 m during drumlin formation, indicating an ice surface slope of 1 m/km. The occurrence of sediments that provided low basal shear stresses, and the orientation of drumlins and megaflutes indicating ice confluence both point to high glacier flow velocities and suggest that an ice stream, rather than a slower moving part of the ice sheet, occupied the Norwegian Channel during the Late Weichselian maximum. Deformation till overlying, more or less, undeformed glaciomarine diamicton suggests that high glacier velocities during periods of low driving stresses were possible due to a subglacial deformable layer. 相似文献
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Bedrock surfaces exposed around Llyn Llydaw, North Wales demonstrate contrasting styles of erosion beneath a Late Devensian ice sheet and a Loch Lomond Stadial (LLS) valley glacier. Ice sheet erosion involved lee-side fracturing, surface fracture wear and abrasive wear, while LLS erosion was primarily by abrasive wear. Preservation of ice sheet erosional features indicates limited rates of erosion during the LLS. Analysis of the geometry and distribution of erosional markings suggests that the low erosional capacity of the LLS glacier was due to a low basal sliding velocity. This prevented the formation of lee-side cavities, reduced the debris flux over the bed and minimised particle-bed contact loads. Reconstructions of the mass balance and geometry of the LLS glacier indicate that most of its balance velocity could be achieved by internal deformation alone. A combination of low subglacial water pressures and an unusually rough substrate explain the low sliding velocities. High bed roughness is due to the absence of leeside cavities and a change in flow orientation between ice sheet and LLS times, which meant that the LLS glacier was in contact with roughness elements which were generated in cavities beneath the ice sheet. 相似文献
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The rock glacier Innere Ölgrube, located in a small side valley of the Kauner Valley (Ötztal Alps, Austria), consists of two separate, tongue-shaped rock glaciers lying next to each other. Investigations indicate that both rock glaciers contain a core of massive ice. During winter, the temperature at the base of the snow cover (BTS) is significantly lower at the active rock glacier than on permafrost-free ground adjacent to the rock glacier. Discharge is characterized by strong seasonal and diurnal variations, and is strongly controlled by the local weather conditions. Water temperature of the rock glacier springs remains constantly low, mostly below 1°C during the whole melt season. The morphology of the rock glaciers and the presence of meltwater lakes in their rooting zones as well as the high surface flow velocities of >1 m/yr point to a glacial origin. The northern rock glacier, which is bounded by lateral moraines, evolved from the debris-covered tongue of a small glacier of the Little Ice Age with its last highstand around A.D. 1850. Due to the global warming in the following decades, the upper parts of the steep and debris-free ice glacier melted, whereas the debris-covered glacier tongue transformed into an active rock glacier. Due to this evolution and due to the downslope movement, the northern rock glacier, although still active, at present is cut off from its ice and debris supply. The southern rock glacier has developed approximately during the same period from a debris-covered cirque glacier at the foot of the Wannetspitze massif. 相似文献
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《Earth》2007,83(3-4):143-179
Calving of icebergs is an important component of mass loss from the polar ice sheets and glaciers in many parts of the world. Calving rates can increase dramatically in response to increases in velocity and/or retreat of the glacier margin, with important implications for sea level change. Despite their importance, calving and related dynamic processes are poorly represented in the current generation of ice sheet models. This is largely because understanding the ‘calving problem’ involves several other long-standing problems in glaciology, combined with the difficulties and dangers of field data collection. In this paper, we systematically review different aspects of the calving problem, and outline a new framework for representing calving processes in ice sheet models. We define a hierarchy of calving processes, to distinguish those that exert a fundamental control on the position of the ice margin from more localised processes responsible for individual calving events. The first-order control on calving is the strain rate arising from spatial variations in velocity (particularly sliding speed), which determines the location and depth of surface crevasses. Superimposed on this first-order process are second-order processes that can further erode the ice margin. These include: fracture propagation in response to local stress imbalances in the immediate vicinity of the glacier front; undercutting of the glacier terminus by melting at or below the waterline; and bending at the junction between grounded and buoyant parts of an ice tongue. Calving of projecting, submerged ‘ice feet’ can be regarded as a third-order process, because it is paced by first- or second-order calving above the waterline.First-order calving can be represented in glacier models using a calving criterion based on crevasse depth, which is a function of longitudinal strain rate. Modelling changes in terminus position and calving rates thus reduces to the problem of determining the ice geometry and velocity distribution. Realistic solutions to the problem of modelling ice flow therefore depend critically on an appropriate choice of sliding law. Models that assume that basal velocities are controlled by basal drag can replicate much of the observed behaviour of calving glaciers with grounded termini, but an important limitation is that they cannot be used to model floating glacier termini or ice shelves. Alternative sliding laws that parameterise drag from the glacier margins provide more flexible and robust ways of representing calving in ice sheet models. Such models can explain a remarkable range of observed phenomena within a simple, unifying framework, including: downglacier increases in velocity and strain rates where basal and/or lateral drag diminishes; flow acceleration in response to thinning through time; the tendency for glaciers to stabilise at ‘pinning points’ in relatively shallow water or fjord narrowings; the constraints on ice shelf stability; and the contrasts in calving rates between tidewater and freshwater calving glaciers. Many unresolved issues remain, however, including the role played by the removal of backstress in the acceleration of retreating calving glaciers, and the controls on melting at and below the waterline. 相似文献
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Evidence for former fast glacier flow (ice streaming) in the southwest Laurentide Ice Sheet is identified on the basis of regional glacial geomorphology and sedimentology, highlighting the depositional processes associated with the margin of a terrestrial terminating ice stream. Preliminary mapping from a digital elevation model of Alberta identifies corridors of smoothed topography and corridor‐parallel streamlined landforms (megaflutes to mega‐lineations) that display high levels of spatial coherency. Ridges that lie transverse to the dominant streamlining patterns are interpreted as: (a) series of minor recessional push moraines; (b) thrust block moraines or composite ridges/hill–hole pairs constructed during readvances/surges; and (c) overridden moraines (cupola hills), apparently of thrust origin. Together these landforms demarcate the beds and margins of former fast ice flow trunks or ice streams that terminated as lobate forms. Localised cross‐cutting and/or misalignment of flow sets indicates temporal separation and the overprinting of ice streams/lobes. The fast‐flow tracks are separated by areas of interlobate or inter‐stream terrain in which moraines have been constructed at the margins of neighbouring (competing) ice streams/outlet glaciers; this inter‐stream terrain was covered by more sluggish, non‐streaming ice during full glacial conditions. Thin tills at the centres of the fast‐flow corridors, in many places unconformably overlying stratified sediments, suggest that widespread till deformation may have been subordinate to basal sliding in driving fast ice flow but the general thickening of tills towards the lobate terminal margins of ice streams/outlet glaciers is consistent with subglacial deformation theory. In this area of relatively low relief we speculate that fast glacier flow or streaming was highly dynamic and transitory, sometimes with fast‐flowing trunks topographically fixed in their onset zones and with the terminus migrating laterally. The occurrence of minor push moraines and flutings and associated landforms, because of their similarity to modern active temperate glacial landsystems, are interpreted as indicative of ice lobe marginal oscillations, possibly in response to seasonal climatic forcing, in locations where meltwater was more effectively drained from the glacier bed. Further north, the occurrence of surging glacier landsystems suggests that persistent fast glacier flow gave way to more transitory surging, possibly in response to the decreasing size of ice reservoir areas in dispersal centres and also locally facilitated by ice‐bed decoupling and drawdown initiated by the development of ice‐dammed lakes. Copyright © 2008 John Wiley & Sons, Ltd. 相似文献
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冰芯高分辨率高保真地记录了过去不同时间尺度气候环境变化历史,而冰芯精确定年是重建过去气候环境演化的先决条件。通过回顾青藏高原冰芯定年的常用方法,提出了目前冰芯定年仍存在的挑战和机遇。通常的冰芯定年方法包括基于冰芯季节变化信号的数年层方法、放射性标志层定年、冰川流动模型、基于其他已知时间序列的对比定年,以及放射性同位素定年。最可靠的方法是数年层的方法,但受到冰川中下部年层逐渐减薄的制约,冰川流动模型主要应用于冰芯中下部定年,但存在不确定性较大而且难以验证的难题。未来冰芯学科发展对冰芯定年提出了更高要求,随着测量技术与手段的突破,新的方法与技术开始在极地冰芯与高山冰芯定年研究中展示了广泛的应用前景。冰芯连续测量技术(如冰芯同位素连续测量技术、激光剥蚀等离子体质谱技术)大幅度提高了冰芯测量结果的时间精度,有可能把数年层的定年方法延推到冰芯底部;基于“原子阱痕量分析”(Atom Trap Trace Analysis,ATTA)的惰性气体(Kr、Kr、Ar)放射性测年技术是一项革命性的技术,由于惰性气体在大气中的稳定性与均匀性使其在不同时间尺度冰川冰的绝对定年中发挥出优势。低浓度的可溶性有机碳的14C定年也从实验室探索阶段开始转入试用阶段,而且用冰量低,有望解决冰芯中碳含量低,定年困难的窘迫状况。此外,人类活动影响之前处于自然背景下的冰芯3H低本底测量技术结合数据处理方法,有望恢复过去100~200年与太阳活动周期相关的信号,将补充放射性标志层只有近代结果的不足。这些新的技术与方法在冰芯定年中的应用有望进一步推动中低纬度高山冰芯研究。 相似文献